Publications of Mark C. Kruse :recent first combined listing:
%% Papers Published
@article{fds376030,
Author = {ATLAS Collaboration},
Title = {A detailed map of Higgs boson interactions by the ATLAS
experiment ten years after the discovery.},
Journal = {Nature},
Volume = {607},
Number = {7917},
Pages = {52-59},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {July},
url = {http://dx.doi.org/10.1038/s41586-022-04893-w},
Abstract = {The standard model of particle physics<sup>1-4</sup>
describes the known fundamental particles and forces that
make up our Universe, with the exception of gravity. One of
the central features of the standard model is a field that
permeates all of space and interacts with fundamental
particles<sup>5-9</sup>. The quantum excitation of this
field, known as the Higgs field, manifests itself as the
Higgs boson, the only fundamental particle with no spin. In
2012, a particle with properties consistent with the Higgs
boson of the standard model was observed by the ATLAS and
CMS experiments at the Large Hadron Collider at
CERN<sup>10,11</sup>. Since then, more than 30 times as
many Higgs bosons have been recorded by the ATLAS
experiment, enabling much more precise measurements and new
tests of the theory. Here, on the basis of this larger
dataset, we combine an unprecedented number of production
and decay processes of the Higgs boson to scrutinize its
interactions with elementary particles. Interactions with
gluons, photons, and W and Z bosons-the carriers of the
strong, electromagnetic and weak forces-are studied in
detail. Interactions with three third-generation matter
particles (bottom (b) and top (t) quarks, and tau leptons
(τ)) are well measured and indications of interactions with
a second-generation particle (muons, μ) are emerging. These
tests reveal that the Higgs boson discovered ten years ago
is remarkably consistent with the predictions of the theory
and provide stringent constraints on many models of new
phenomena beyond the standard model.},
Doi = {10.1038/s41586-022-04893-w},
Key = {fds376030}
}
@article{fds327148,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {A measurement of material in the ATLAS tracker using
secondary hadronic interactions in 7TeV pp
collisions},
Journal = {Journal of Instrumentation},
Volume = {11},
Number = {11},
Pages = {P11020-P11020},
Publisher = {IOP Publishing},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1088/1748-0221/11/11/P11020},
Abstract = {Knowledge of the material in the ATLAS inner tracking
detector is crucial in understanding the reconstruction of
charged-particle tracks, the performance of algorithms that
identify jets containing b-hadrons and is also essential to
reduce background in searches for exotic particles that can
decay within the inner detector volume. Interactions of
primary hadrons produced in pp collisions with the material
in the inner detector are used to map the location and
amount of this material. The hadronic interactions of
primary particles may result in secondary vertices, which in
this analysis are reconstructed by an inclusive
vertex-finding algorithm. Data were collected using
minimum-bias triggers by the ATLAS detector operating at the
LHC during 2010 at centre-of-mass energy √s = 7TeV, and
correspond to an integrated luminosity of 19nb-1. Kinematic
properties of these secondary vertices are used to study the
validity of the modelling of hadronic interactions in
simulation. Secondary-vertex yields are compared between
data and simulation over a volume of about 0.7 m3 around the
interaction point, and agreement is found within overall
uncertainties.},
Doi = {10.1088/1748-0221/11/11/P11020},
Key = {fds327148}
}
@article{fds314158,
Author = {al, TAE and Collaboration, TCDF},
Title = {A Measurement of sin 2 from B with the CDF
Detector},
Journal = {Phys. Rev.},
Volume = {D61},
Number = {7},
Pages = {072005},
Year = {2000},
ISSN = {0556-2821},
Abstract = {This paper reports an updated measurement of the standard
model CP violation parameter sin 2β using the CDF Detector
at Fermilab. The entire run I data sample of 110 pb -1 of
proton-antiproton collisions at √s = 1.8 TeV is used to
identify a signal sample of ∼400 B→J/φK s0 events,
where J/φ→μ + μ - →μ + μ - . The flavor of the
neutral B meson is identified at the time of production by
combining information from three tagging algorithms: a
same-side tag, a jet-charge tag, and a soft-lepton tag. A
maximum likelihood fitting method is used to determine sin
2β=0.79 -0.44+0.41 (stat+syst). This value of sin 2β is
consistent with the standard model prediction, based upon
existing measurements, of a large positive CP-violating
asymmetry in this decay mode. ©2000 The American Physical
Society.},
Key = {fds314158}
}
@article{fds321365,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, MF and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
M},
Title = {A measurement of the ratio of the production cross sections
for [Formula: see text] and [Formula: see text] bosons in
association with jets with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {12},
Pages = {3168},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3168-9},
Abstract = {The ratio of the production cross sections for [Formula: see
text] and [Formula: see text] bosons in association with
jets has been measured in proton-proton collisions at
[Formula: see text] with the ATLAS experiment at the Large
Hadron Collider. The measurement is based on the entire 2011
dataset, corresponding to an integrated luminosity of
[Formula: see text]. Inclusive and differential
cross-section ratios for massive vector bosons decaying to
electrons and muons are measured in association with jets
with transverse momentum [Formula: see text] and jet
rapidity [Formula: see text]. The measurements are compared
to next-to-leading-order perturbative QCD calculations and
to predictions from different Monte Carlo generators
implementing leading-order matrix elements supplemented by
parton showers.},
Doi = {10.1140/epjc/s10052-014-3168-9},
Key = {fds321365}
}
@article{fds321329,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyka, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa,
C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araquea, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
M and Armbruster, AJ and Arnaez, O and Arnal, V},
Title = {A neural network clustering algorithm for the ATLAS silicon
pixel detector},
Journal = {Journal of Instrumentation},
Volume = {9},
Number = {9},
Pages = {P09009-P09009},
Publisher = {IOP Publishing},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1088/1748-0221/9/09/P09009},
Abstract = {A novel technique to identify and split clusters created by
multiple charged particles in the ATLAS pixel detector using
a set of artificial neural networks is presented. Such
merged clusters are a common feature of tracks originating
from highly energetic objects, such as jets. Neural networks
are trained using Monte Carlo samples produced with a
detailed detector simulation. This technique replaces the
former clustering approach based on a connected component
analysis and charge interpolation. The performance of the
neural network splitting technique is quantified using data
from proton-proton collisions at the LHC collected by the
ATLAS detector in 2011 and from Monte Carlo simulations.
This technique reduces the number of clusters shared between
tracks in highly energetic jets by up to a factor of three.
It also provides more precise position and error estimates
of the clusters in both the transverse and longitudinal
impact parameter resolution.},
Doi = {10.1088/1748-0221/9/09/P09009},
Key = {fds321329}
}
@article{fds315434,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
J},
Title = {A new method to distinguish hadronically decaying boosted
Z bosons from W bosons using the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {238},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4065-1},
Abstract = {The distribution of particles inside hadronic jets produced
in the decay of boosted <i>W</i> and <i>Z</i> bosons can be
used to discriminate such jets from the continuum
background. Given that a jet has been identified as likely
resulting from the hadronic decay of a boosted <i>W</i> or
<i>Z</i> boson, this paper presents a technique for further
differentiating <i>Z</i> bosons from <i>W</i> bosons. The
variables used are jet mass, jet charge, and a
<i>b</i>-tagging discriminant. A likelihood tagger is
constructed from these variables and tested in the
simulation of [Formula: see text] for bosons in the
transverse momentum range 200 GeV [Formula: see
text] 400 GeV in [Formula: see text] TeV <i>pp</i>
collisions with the ATLAS detector at the LHC. For
<i>Z</i>-boson tagging efficiencies of [Formula: see text],
50, and [Formula: see text], one can achieve [Formula: see
text]-boson tagging rejection factors ([Formula: see text])
of 1.7, 8.3 and 1000, respectively. It is not possible to
measure these efficiencies in the data due to the lack of a
pure sample of high [Formula: see text], hadronically
decaying <i>Z</i> bosons. However, the modelling of the
tagger inputs for boosted <i>W</i> bosons is studied in data
using a [Formula: see text]-enriched sample of events in
20.3 fb[Formula: see text] of data at [Formula: see text]
TeV. The inputs are well modelled within uncertainties,
which builds confidence in the expected tagger
performance.},
Doi = {10.1140/epjc/s10052-016-4065-1},
Key = {fds315434}
}
@article{fds321186,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {A search for an excited muon decaying to a muon and two jets
in pp collisions at √ s = 8 TeV with the ATLAS
detector},
Journal = {New Journal of Physics},
Volume = {18},
Number = {7},
Pages = {073021-073021},
Publisher = {IOP Publishing},
Year = {2016},
Month = {July},
url = {http://dx.doi.org/10.1088/1367-2630/18/7/073021},
Abstract = {Anew search signature for excited leptons is explored.
Excited muons are sought in the channel pp → μμ∗→
μμ jet jet, assuming both the production and decay occur
via a contact interaction. The analysis is based on 20.3
fb-1 of pp collision data at a centre-of-mass energy of s =
8 TeV taken with the ATLAS detector at the large hadron
collider. No evidence of excited muons is found, and limits
are set at the 95% confidence level on the cross section
times branching ratio as a function of the excited-muonmass
μμ∗. For μμ∗between 1.3 and 3.0 TeV, the upper limit
on φB (μ∗→ μqq) is between 0.6 and 1 fb. Limits on sB
are converted to lower bounds on the compositeness scale. In
the limiting case L = μμ∗, excitedmuonswith amass
below2.8 TeVare excluded.With the samemodel assumptions,
these limits at larger μ∗masses improve upon previous
limits fromtraditional searches based on the gauge-mediated
decay μ∗→ μγ.},
Doi = {10.1088/1367-2630/18/7/073021},
Key = {fds321186}
}
@article{fds308809,
Author = {Collaboration, CDF},
Title = {A Search for B - B Oscillations Using the Semileptonic Decay
B -> o;=Xu},
Journal = {Phys. Rev. Lett.},
Volume = {82},
Number = {18},
Pages = {3576},
Year = {1999},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.3576},
Abstract = {A search for Bs0-B̄s0 oscillations is performed in a sample
of Bs0 semileptonic decays collected using dilepton triggers
at the Tevatron Collider during 1992-1995. The Bs0 is
reconstructed using φ mesonlepton correlations; its initial
production flavor is determined with the second lepton in
the event. From a signal of 1068 with a Bs0 purity of 61%,
we obtain a limit on the Bs0-B̄s0 oscillation frequency of
Δms > 5.8 ps-1 at 95% confidence level. © 1999 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.82.3576},
Key = {fds308809}
}
@article{fds308348,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, R and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia,
A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, R and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Gimenez, VC and Castro,
NF and Cataldi, G and Catastini, R and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, R and Citron, ZH and Citterio, M and Ciubancan, M and Clark,
A},
Title = {A search for high-mass resonances decaying to
τ+τ- in pp collisions at
√s=7 TeV with the ATLAS detector},
Journal = {PHYSICS LETTERS B},
Volume = {719},
Number = {4-5},
Pages = {242-260},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.040},
Abstract = {© 2012 CERN This Letter presents a search for high-mass
resonances decaying into τ+τ− final states using
proton-proton collisions at s=7 TeV produced by the Large
Hadron Collider. The data were recorded with the ATLAS
detector and correspond to an integrated luminosity of 4.6
fb−1. No statistically significant excess above the
Standard Model expectation is observed; 95% credibility
upper limits are set on the cross section times branching
fraction of Z′ resonances decaying into τ+τ− pairs as
a function of the resonance mass. As a result, Z′ bosons
of the Sequential Standard Model with masses less than 1.40
TeV are excluded at 95% credibility.},
Doi = {10.1016/j.physletb.2013.01.040},
Key = {fds308348}
}
@article{fds321242,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
M},
Title = {A search for high-mass resonances decaying to
τ+τ− in pp collisions at √s =8
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {7},
Publisher = {Springer Nature},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2015)157},
Abstract = {Abstract: A search for high-mass resonances decaying into
τ+τ− final states using proton-proton collisions at
s=8$$ \sqrt{s}=8 $$ TeV produced by the Large Hadron
Collider is presented. The data were recorded with the ATLAS
detector and correspond to an integrated luminosity of
19.5–20.3 fb−1. No statistically significant excess
above the Standard Model expectation is observed; 95%
credibility upper limits are set on the cross section times
branching fraction of Z′ resonances decaying into τ+τ−
pairs as a function of the resonance mass. As a result, Z′
bosons of the Sequential Standard Model with masses less
than 2.02 TeV are excluded at 95% credibility. The impact of
the fermionic couplings on the Z′ acceptance is
investigated and limits are also placed on a Z′ model that
exhibits enhanced couplings to third-generation
fermions.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP07(2015)157},
Key = {fds321242}
}
@article{fds308349,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung,
C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker,
S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brown, G and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, E and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
J},
Title = {A search for prompt lepton-jets in pp collisions at
√s=7 TeV with the ATLAS detector},
Journal = {PHYSICS LETTERS B},
Volume = {719},
Number = {4-5},
Pages = {299-317},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.034},
Abstract = {© 2013 CERN We present a search for a light (mass <2GeV)
boson predicted by Hidden Valley supersymmetric models that
decays into a final state consisting of collimated muons or
electrons, denoted “lepton-jets”. The analysis uses
5fb−1 of s=7TeV proton–proton collision data recorded by
the ATLAS detector at the Large Hadron Collider to search
for the following signatures: single lepton-jets with at
least four muons; pairs of lepton-jets, each with two or
more muons; and pairs of lepton-jets with two or more
electrons. This study finds no statistically significant
deviation from the Standard Model prediction and places 95%
confidence-level exclusion limits on the production cross
section times branching ratio of light bosons for several
parameter sets of a Hidden Valley model.},
Doi = {10.1016/j.physletb.2013.01.034},
Key = {fds308349}
}
@article{fds308666,
Author = {Abulencia, and A, and others},
Title = {A search for scalar bottom quarks from gluino decays in
$\bar{p}p$ collisions at $\sqrt{s} =$ 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {17},
Pages = {171802},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.171802},
Abstract = {We searched for scalar bottom quarks in 156 pb-1 of p anti-p
collisions at s**(1/2) = 1.96 TeV recorded by the CDF II
experiment at the Tevatron. Scalar bottom quarks can be
produced from gluino decays in R-parity conserving models of
supersymmetry when the mass of the gluino exceeds that of
the scalar bottom quark. Then, a scalar bottom quark. Then,
a scalar bottom quark can decay into a bottom quark and a
neutralino. To search for this scenario, we investigated
events with large missing transverse energy and at least
three jets, two or more of which were identified as
containing a secondary vertex from the hadronization of b
quarks. We found four candidate events, where 2.6 +/- 0.7
are expected from standard model processes, and placed 95\%
confidence level lower limits on gluino and scalar bottom
quark masses of up to 280 and 240 GeV/c2,
respectively.},
Doi = {10.1103/physrevlett.96.171802},
Key = {fds308666}
}
@article{fds308678,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH},
Title = {A search for t → τ ν q in t over(t, ̄)
production},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {639},
Number = {3-4},
Pages = {172-178},
Publisher = {Elsevier BV},
Year = {2006},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2006.06.030},
Abstract = {We present a search for t over(t, ̄) events with a tau
lepton in the final state. The data sample corresponds to an
integrated luminosity of 194 pb-1 collected with the CDF II
detector from p over(p, ̄) collisions at a center of mass
energy of 1.96 TeV. We observe two events with an expected
signal of 1.0 ± 0.2 events and a background of 1.3 ± 0.3
events. We determine a 95% confidence level upper limit on
rτ, the ratio of the measured rate of t → τ ν q to the
expectation, of 5.2. © 2006 Elsevier B.V. All rights
reserved.},
Doi = {10.1016/j.physletb.2006.06.030},
Key = {fds308678}
}
@article{fds365387,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {A search for the decays of stopped long-lived particles at
√s = 13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2021)173},
Abstract = {A search for long-lived particles, which have come to rest
within the ATLAS detector, is presented. The subsequent
decays of these particles can produce high-momentum jets,
resulting in large out-of-time energy deposits in the ATLAS
calorimeters. These de- cays are detected using data
collected during periods in the LHC bunch structure when
collisions are absent. The analysed dataset is composed of
events from proton-proton collisions produced by the Large
Hadron Collider at a centre-of-mass energy of s = 13 TeV and
recorded by the ATLAS experiment during 2017 and 2018. The
dataset used for this search corresponds to a total live
time of 579 hours. The results of this search are used to
derive lower limits on the mass of gluino R-hadrons,
assuming a branching fraction B(g~→qq¯χ10) = 100%, with
masses of up to 1.4 TeV excluded for gluino lifetimes of
10−5 to 103 s. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP07(2021)173},
Key = {fds365387}
}
@article{fds308479,
Author = {Aaltonen, and T, and others},
Title = {A Search for the Higgs Boson Using Neural Networks in Events
with Missing Energy and $b$-quark Jets in $p\bar p$
Collisions at $\sqrt{s}=1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {14},
Pages = {141801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.141801},
Abstract = {http://arxiv.org/abs/0911.3935},
Doi = {10.1103/PhysRevLett.104.141801},
Key = {fds308479}
}
@article{fds321195,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {A search for top squarks with R-parity-violating decays to
all-hadronic final states with the ATLAS detector in √s =
8 TeV proton-proton collisions},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {6},
Pages = {1-49},
Publisher = {Springer Nature},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2016)067},
Abstract = {A search for the pair production of top squarks, each with
R-parity-violating decays into two Standard Model quarks, is
performed using 17.4 fb−1 of √s = 8 TeV proton-proton
collision data recorded by the ATLAS experiment at the LHC.
Each top squark is assumed to decay to a b- and an s-quark,
leading to four quarks in the final state. Background
discrimination is achieved with the use of b-tagging and
selections on the mass and substructure of large-radius
jets, providing sensitivity to top squark masses as low as
100 GeV. No evidence of an excess beyond the Standard Model
background prediction is observed and top squarks decaying
to b¯ s¯ are excluded for top squark masses in the range
100 ≤ mt≤ 315 GeV at 95% confidence level.},
Doi = {10.1007/JHEP06(2016)067},
Key = {fds321195}
}
@article{fds315439,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {A search for tt resonances using lepton-plus-jets events in
proton-proton collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {8},
Publisher = {Springer Nature},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2015)148},
Abstract = {Abstract: A search for new particles that decay into top
quark pairs is reported. The search is performed with the
ATLAS experiment at the LHC using an integrated luminosity
of 20.3 fb−1 of proton-proton collision data collected at
a centre-of-mass energy of √s=8 TeV. The lepton-plus-jets
final state is used, where the top pair decays to
W+bW−b¯, with one W boson decaying leptonically and the
other hadronically. The invariant mass spectrum of top quark
pairs is examined for local excesses or deficits that are
inconsistent with the Standard Model predictions. No
evidence for a top quark pair resonance is found, and 95%
confidence-level limits on the production rate are
determined for massive states in benchmark models. The upper
limits on the cross-section times branching ratio of a
narrow Z′ boson decaying to top pairs range from 4.2 pb to
0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A
narrow leptophobic topcolour Z′ boson with mass below 1.8
TeV is excluded. Upper limits are set on the cross-section
times branching ratio for a broad colour-octet resonance
with Γ/m = 15% decaying to tt¯. These range from 4.8 pb to
0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza-Klein
excitation of the gluon in a Randall-Sundrum model is
excluded for masses below 2.2 TeV.},
Doi = {10.1007/JHEP08(2015)148},
Key = {fds315439}
}
@article{fds308502,
Author = {Aaltonen, and T, and others},
Title = {A study of the associated production of photons and
$b$-quark jets in $p \bar{p}$ collisions at $\sqrt{s} =
1.96$ TeV},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {5},
Pages = {052006},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.052006},
Abstract = {http://arxiv.org/abs/0912.3453},
Doi = {10.1103/PhysRevD.81.052006},
Key = {fds308502}
}
@article{fds308771,
Author = {Apollinari, G and Barone, M and Benjamin, D and Carithers, W and Dorigo,
T and Fiori, I and Franklin, M and Giromini, P and Happacher, F and Konigsberg, J and Kruse, M and Miscetti, S and Parri, A and Ptohos, F and Velev, G},
Title = {Additional studies of the probability that the events with a
superjet observed by CDF are consistent with the SM
prediction},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {65},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.65.032004},
Abstract = {In the (Formula presented) jet data collected by Collider
Detector at Fermilab during the 1992–1995 Fermilab
collider run, 13 events were observed to contain a superjet
when (Formula presented) events are expected. A previous
article detailed the selection and the kinematical
properties of these events. The present paper provides
estimates of the probability that the kinematics of these 13
events is statistically consistent with the standard model
prediction. © 2002 The American Physical
Society.},
Doi = {10.1103/PhysRevD.65.032004},
Key = {fds308771}
}
@article{fds365419,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Alignment of the ATLAS Inner Detector in Run
2},
Journal = {European Physical Journal C},
Volume = {80},
Number = {12},
Year = {2020},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08700-6},
Abstract = {The performance of the ATLAS Inner Detector alignment has
been studied using pp collision data at s=13TeV collected by
the ATLAS experiment during Run 2 (2015–2018) of the Large
Hadron Collider (LHC). The goal of the detector alignment is
to determine the detector geometry as accurately as possible
and correct for time-dependent movements. The Inner Detector
alignment is based on the minimization of track-hit
residuals in a sequence of hierarchical levels, from global
mechanical assembly structures to local sensors. Subsequent
levels have increasing numbers of degrees of freedom; in
total there are almost 750,000. The alignment determines
detector geometry on both short and long timescales, where
short timescales describe movements within an LHC fill. The
performance and possible track parameter biases originating
from systematic detector deformations are evaluated.
Momentum biases are studied using resonances decaying to
muons or to electrons. The residual sagitta bias and
momentum scale bias after alignment are reduced to less than
∼0.1TeV-1 and 0.9 × 10 - 3, respectively. Impact
parameter biases are also evaluated using tracks within
jets.},
Doi = {10.1140/epjc/s10052-020-08700-6},
Key = {fds365419}
}
@article{fds308420,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan,
A and Arisawa, T and Artikov, A and Ashmanskas, W and Auerbach, B and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Calancha, C and Campanelli, M and Campbell, M and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cerri, A and Cerrito, L and Chen, YC and Chiarelli, G and Chlachidze,
G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De
Cecco, S and Dell'Orso, M and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M},
Title = {An additional study of multi-muon events produced in pp-
collisions at s=1.96 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {710},
Number = {2},
Pages = {278-283},
Publisher = {Elsevier BV},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2012.02.081},
Abstract = {We present one additional study of multi-muon events
produced at the Fermilab Tevatron collider and recorded by
the CDF II detector. We use a data set acquired with a
dedicated dimuon trigger and corresponding to an integrated
luminosity of 3.9 fb -1. We investigate the distribution of
the azimuthal angle between the two trigger muons in events
containing at least four additional muon candidates to test
the compatibility of these events with originating from
known QCD processes. We find that this distribution is
markedly different from what is expected from such QCD
processes and this observation strongly disfavors the
possibility that multi-muon events result from an
underestimate of the rate of misidentified muons in ordinary
QCD events. © 2012 Elsevier B.V.},
Doi = {10.1016/j.physletb.2012.02.081},
Key = {fds308420}
}
@article{fds308631,
Author = {Abulencia, and A, and others},
Title = {Analysis of the quantum numbers J(PC) of the
X(3872)},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {13},
Pages = {132002},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.132002},
Abstract = {We present an analysis of angular distributions and
correlations of the X(3872) particle in the exclusive decay
mode X(3872)-->J/psipi+pi- with J/psi-->µ+µ-. We use 780
pb-1 of data from p[overline p] collisions at sqrt(s)=1.96
TeV collected with the CDF II detector at the Fermilab
Tevatron. We derive constraints on spin, parity, and charge
conjugation parity of the X(3872) particle by comparing
measured angular distributions of the decay products with
predictions for different JPC hypotheses. The assignments
JPC=1++ and 2-+ are the only ones consistent with the
data.},
Doi = {10.1103/physrevlett.98.132002},
Key = {fds308631}
}
@article{fds375908,
Author = {Amerl, M and Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi,
G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori,
G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang,
R and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Ghosh, A and Johns,
KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK},
Title = {Anomaly detection search for new resonances decaying into a
Higgs boson and a generic new particle X in hadronic final
states using Formula Presented pp collisions with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {108},
Number = {5},
Year = {2023},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.108.052009},
Abstract = {A search is presented for a heavy resonance Formula
Presented decaying into a Standard Model Higgs boson Formula
Presented and a new particle Formula Presented in a fully
hadronic final state. The full Large Hadron Collider run 2
dataset of proton-proton collisions at Formula Presented
collected by the ATLAS detector from 2015 to 2018 is used
and corresponds to an integrated luminosity of Formula
Presented. The search targets the high Formula
Presented-mass region, where the Formula Presented and
Formula Presented have a significant Lorentz boost in the
laboratory frame. A novel application of anomaly detection
is used to define a general signal region, where events are
selected solely because of their incompatibility with a
learned background-only model. It is constructed using a
jet-level tagger for signal-model-independent selection of
the boosted Formula Presented particle, representing the
first application of fully unsupervised machine learning to
an ATLAS analysis. Two additional signal regions are
implemented to target a benchmark Formula Presented decay
into two quarks, covering topologies where the Formula
Presented is reconstructed as either a single large-radius
jet or two small-radius jets. The analysis selects Higgs
boson decays into Formula Presented, and a dedicated
neural-network-based tagger provides sensitivity to the
boosted heavy-flavor topology. No significant excess of data
over the expected background is observed, and the results
are presented as upper limits on the production cross
section Formula Presented) for signals with Formula
Presented between 1.5 and 6 TeV and Formula Presented
between 65 and 3000 GeV.},
Doi = {10.1103/PhysRevD.108.052009},
Key = {fds375908}
}
@article{fds321307,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amaral
Coutinho, Y and Amelung, C and Amor Dos Santos and SP and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B},
Title = {ATLAS Collaboration},
Journal = {Nuclear Physics A},
Volume = {932},
Pages = {572-594},
Publisher = {Elsevier BV},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1016/S0375-9474(14)00601-0},
Doi = {10.1016/S0375-9474(14)00601-0},
Key = {fds321307}
}
@article{fds321142,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {ATLAS Collaboration},
Journal = {Nuclear Physics A},
Volume = {956},
Pages = {922-944},
Publisher = {Elsevier BV},
Year = {2016},
Month = {December},
url = {http://dx.doi.org/10.1016/S0375-9474(16)30232-9},
Doi = {10.1016/S0375-9474(16)30232-9},
Key = {fds321142}
}
@article{fds329807,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {ATLAS Collaboration},
Journal = {Nuclear Physics A},
Volume = {967},
Pages = {942-964},
Publisher = {Elsevier BV},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1016/S0375-9474(17)30376-7},
Doi = {10.1016/S0375-9474(17)30376-7},
Key = {fds329807}
}
@article{fds375936,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport, PP and Aloisio,
A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev,
V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {ATLAS flavour-tagging algorithms for the LHC Run 2 pp
collision dataset},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11699-1},
Abstract = {The flavour-tagging algorithms developed by the ATLAS
Collaboration and used to analyse its dataset of s=13 TeV pp
collisions from Run 2 of the Large Hadron Collider are
presented. These new tagging algorithms are based on
recurrent and deep neural networks, and their performance is
evaluated in simulated collision events. These developments
yield considerable improvements over previous jet-flavour
identification strategies. At the 77% b-jet identification
efficiency operating point, light-jet (charm-jet) rejection
factors of 170 (5) are achieved in a sample of simulated
Standard Model tt¯ events; similarly, at a c-jet
identification efficiency of 30%, a light-jet (b-jet)
rejection factor of 70 (9) is obtained.},
Doi = {10.1140/epjc/s10052-023-11699-1},
Key = {fds375936}
}
@article{fds365351,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari,
N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C},
Title = {AtlFast3: The Next Generation of Fast Simulation in
ATLAS},
Journal = {Computing and Software for Big Science},
Volume = {6},
Number = {1},
Year = {2022},
Month = {December},
url = {http://dx.doi.org/10.1007/s41781-021-00079-7},
Abstract = {The ATLAS experiment at the Large Hadron Collider has a
broad physics programme ranging from precision measurements
to direct searches for new particles and new interactions,
requiring ever larger and ever more accurate datasets of
simulated Monte Carlo events. Detector simulation with
Geant4 is accurate but requires significant CPU resources.
Over the past decade, ATLAS has developed and utilized tools
that replace the most CPU-intensive component of the
simulation—the calorimeter shower simulation—with faster
simulation methods. Here, AtlFast3, the next generation of
high-accuracy fast simulation in ATLAS, is introduced.
AtlFast3 combines parameterized approaches with
machine-learning techniques and is deployed to meet current
and future computing challenges, and simulation needs of the
ATLAS experiment. With highly accurate performance and
significantly improved modelling of substructure within
jets, AtlFast3 can simulate large numbers of events for a
wide range of physics processes.},
Doi = {10.1007/s41781-021-00079-7},
Key = {fds365351}
}
@article{fds375899,
Author = {ATLAS Collaboration},
Title = {Author Correction: A detailed map of Higgs boson
interactions by the ATLAS experiment ten years after the
discovery.},
Journal = {Nature},
Volume = {623},
Number = {7985},
Pages = {E5},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1038/s41586-023-06248-5},
Doi = {10.1038/s41586-023-06248-5},
Key = {fds375899}
}
@article{fds323673,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arduini, G and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Beam-induced and cosmic-ray backgrounds observed in the
ATLAS detector during the LHC 2012 proton-proton running
period},
Journal = {Journal of Instrumentation},
Volume = {11},
Number = {5},
Pages = {P05013-P05013},
Publisher = {IOP Publishing},
Year = {2016},
Month = {May},
url = {http://dx.doi.org/10.1088/1748-0221/11/05/P05013},
Abstract = {This paper discusses various observations on beam-induced
and cosmic-ray backgrounds in the ATLAS detector during the
LHC 2012 proton-proton run. Building on published results
based on 2011 data, the correlations between background and
residual pressure of the beam vacuum are revisited. Ghost
charge evolution over 2012 and its role for backgrounds are
evaluated. New methods to monitor ghost charge with beam-gas
rates are presented and observations of LHC abort gap
population by ghost charge are discussed in detail. Fake
jets from colliding bunches and from ghost charge are
analysed with improved methods, showing that ghost charge in
individual radio-frequency buckets of the LHC can be
resolved. Some results of two short periods of dedicated
cosmic-ray background data-taking are shown; in particular
cosmic-ray muon induced fake jet rates are compared to Monte
Carlo simulations and to the fake jet rates from beam
background. A thorough analysis of a particular LHC fill,
where abnormally high background was observed, is presented.
Correlations between backgrounds and beam intensity losses
in special fills with very high β∗ are
studied.},
Doi = {10.1088/1748-0221/11/05/P05013},
Key = {fds323673}
}
@article{fds375920,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH},
Title = {Calibration of the light-flavour jet mistagging efficiency
of the b-tagging algorithms with Z+jets events using 139 fb
- 1 of ATLAS proton–proton collision data at
√s=13 TeV},
Journal = {European Physical Journal C},
Volume = {83},
Number = {8},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11736-z},
Abstract = {The identification of b-jets, referred to as b-tagging, is
an important part of many physics analyses in the ATLAS
experiment at the Large Hadron Collider and an accurate
calibration of its performance is essential for high-quality
physics results. This publication describes the calibration
of the light-flavour jet mistagging efficiency in a data
sample of proton–proton collision events at s=13 TeV
corresponding to an integrated luminosity of 139 fb - 1 .
The calibration is performed in a sample of Z bosons
produced in association with jets. Due to the low mistagging
efficiency for light-flavour jets, a method which uses
modified versions of the b-tagging algorithms referred to as
flip taggers is used in this work. A fit to the
jet-flavour-sensitive secondary-vertex mass is performed to
extract a scale factor from data, to correct the
light-flavour jet mistagging efficiency in Monte Carlo
simulations, while simultaneously correcting the b-jet
efficiency. With this procedure, uncertainties coming from
the modeling of jets from heavy-flavour hadrons are
considerably lower than in previous calibrations of the
mistagging scale factors, where they were dominant. The
scale factors obtained in this calibration are consistent
with unity within uncertainties.},
Doi = {10.1140/epjc/s10052-023-11736-z},
Key = {fds375920}
}
@article{fds308742,
Author = {Akimoto, T and Aoki, M and Azzi, P and Bacchetta, N and Behari, S and Benjamin, D and Bisello, D and Bolla, G and Bortoletto, D and Busetto,
G and Cabrera, S and Canepa, A and Cardoso, G and Chertok, M and Ciobanu,
CI and Derylo, G and Fang, I and Feng, EJ and Fernandez, JP and Flaugher,
B and Freeman, J and Galtieri, L and Galyardt, J and Garcia-Sciveres, M and Giurgiu, G and Haber, C and Hale, D and Hara, K and Harr, R and Hill, C and Hoff, J and Holbrook, B and Hong, SC and Hrycyk, M and Hsiung, TH and Incandela, J and Jeon, EJ and Joo, KK and Junk, T and Kahkola, H and Karjalainen, S and Kim, S and Kobayashi, K and Kong, DJ and Krieger, B and Kruse, M and Kuznetsova, N and Kyre, S and Lander, R and Landry, T and Lauhakangas, R and Lee, J and Lu, RS and Lujan, P and Lukens, P and Mandelli, E and Manea, C and Maksimovic, P and Merkel, P and Min, SN and Moccia, S and Nakano, I and Nelson, T and Nord, B and Novak, J and Okusawa,
T and Orava, R and Orlov, Y and Osterberg, K and Pantano, D and Pavlicek,
V and Pellett, D and Pursley, J and Riipinen, P and Schuyler, B and Shenai,
A and Soha, A and Stuart, D and Tanaka, R and Tavi, M and Von Der Lippe and H and Walder, JP and Wang, Z and Weber, M and Wester, W and Yamamoto, K and Yang,
YC and Yao, W and Yarema, R and Yun, JC and Zetti, F and Zimmerman, T and Zimmermann, S and Zucchelli, S},
Title = {CDF run IIb silicon detector: Electrical performance and
deadtime-less operation},
Journal = {IEEE Transactions on Nuclear Science},
Volume = {51},
Number = {3 III},
Pages = {987-993},
Publisher = {Institute of Electrical and Electronics Engineers
(IEEE)},
Year = {2004},
Month = {June},
url = {http://dx.doi.org/10.1109/TNS.2004.829508},
Abstract = {The main building block and readout unit of the planned CDF
Run lib silicon detector is a "stave," a highly integrated
mechanical, thermal, and electrical structure. One of its
characteristic features is a copper-on-Kapton flexible cable
for power, high voltage, data transmission, and control
signals that is placed directly below the silicon microstrip
sensors. The dense packaging makes deadtime-less operation
of the stave a challenge since coupling of bus cable
activity into the silicon sensors must be suppressed
efficiently. The stave design features relevant for
deadtime-less operation are discussed. The electrical
performance achieved with stave prototypes is
presented.},
Doi = {10.1109/TNS.2004.829508},
Key = {fds308742}
}
@article{fds308746,
Author = {Merkel, P and Azzi, P and Bacchetta, N and Bisello, D and Busetto, G and Hara, K and Kim, S and Manea, C and Wang, Z and Behari, S and Maksimovic,
P and Benjamin, D and Cabrera, S and Kruse, M and Bolla, G and Bortoletto,
D and Canepa, A and Fernandez, JP and Booth, P and Cooke, P and Cascella,
M and Cardoso, G and Derylo, G and Flaugher, B and Hrycyk, M and Kuznetsova, N and Lukens, P and Nelson, T and Orlov, Y and Wester, W and Yun, JC and Chertok, M and Holbrook, B and Lander, R and Landry, T and Pellett, D and Soha, A and Yao, W and Ciobanu, CI and Junk, T and Feng, EJ and Freeman, J and Galtieri, L and Garcia-Sciveres, M and Haber, C and Lujan, PJ and Mandelli, E and Weber, M and Zetti, F and Zimmermann, S and Goldstein, J and Harr, R and Hill, C and Himmel, A and Incandela, J and Stuart, D and Kobayashi, K and Nakano, I and Tanaka, R and Kong, DJ and Yang, YC and Lauhakangas, R and Orava, R and Osterberg, K and Lu, RS and Min, SN and Okusawa, T and Yamamoto, K and Tavi, M and Zucchelli, S and Hong, SC and Jeon, EJ and Too, KK and Lee, J},
Title = {CDF run IIb silicon detector: The innermost
layer},
Journal = {IEEE Transactions on Nuclear Science},
Volume = {51},
Number = {5 I},
Pages = {2215-2219},
Publisher = {Institute of Electrical and Electronics Engineers
(IEEE)},
Year = {2004},
Month = {October},
url = {http://dx.doi.org/10.1109/TNS.2004.835876},
Abstract = {The innermost layer (L00) of the Run IIa silicon detector of
CDF was planned to be replaced for the high luminosity
Tevatron upgrade of Run IIb. This new silicon layer (L0) is
designed to be a radiation tolerant replacement for the
otherwise very similar L00 from Run IIa. The data are read
out via long, fine-pitch, low-mass cables allowing the
hybrids with the chips to sit at higher z(∼ 70 cm),
outside of the tracking volume. The design and first results
from the prototyping phase are presented. Special focus is
placed on the amount and the structure of induced noise as
well as sisnal-to-noise values.},
Doi = {10.1109/TNS.2004.835876},
Key = {fds308746}
}
@article{fds308745,
Author = {Lu, RS and Akimoto, T and Aoki, M and Azzi, P and Bacchetta, N and Behari,
S and Benjamin, D and Bisello, D and Bolla, G and Bortoletto, D and Busetto, G and Cabrera, S and Canepa, A and Cardoso, G and Chertok, M and Ciobanu, CI and Derylo, G and Fang, I and Feng, EJ and Fernandez, JP and Flaugher, B and Freeman, J and Galtieri, L and Galyardt, J and Garcia-Sciveres, M and Giurgiu, G and Haber, C and Hale, D and Hara, K and Harr, R and Hill, C and Hoff, J and Holbrook, B and Hong, SC and Hrycyk, M and Hsiung, TH and Incandela, J and Jeon, EJ and Joo, KK and Junk, T and Kahkola, H and Karjalainen, S and Kim, S and Kobayashi, K and Kong, DJ and Krieger, B and Kruse, M and Kuznetsova, N and Kyre, S and Lander, R and Landry, T and Lauhakangas, R and Lee, J and Lujan, PJ and Lukens, P and Mandelli, E and Manea, C and Maksimovic, P and Merkel, P and Min, SN and Moccia, S and Nakano, I and Nelson, T and Nord, B and Novak, J and Okusawa,
T and Orava, R and Orlov, Y and Osterberg, K and Pantano, D and Pavlicek,
V and Pellett, D and Pursley, J and Riipinen, P and Schuyler, B and Shenai,
A and Soha, A and Stuart, D and Tanaka, R and Tavi, M and Von Der Lippe and H and Walder, JP and Wang, Z and Weber, M and Wester, W and Yamamoto, K and Yang,
YC and Yao, W and Yarema, R and Yun, JC and Zetti, F and Zimmerman, T and Zimmermann, S and Zucchelli, S},
Title = {CDF run IIb silicon: Design and testing},
Journal = {IEEE Transactions on Nuclear Science},
Volume = {51},
Number = {5 I},
Pages = {2209-2214},
Publisher = {Institute of Electrical and Electronics Engineers
(IEEE)},
Year = {2004},
Month = {October},
url = {http://dx.doi.org/10.1109/TNS.2004.835715},
Abstract = {The various generations of Silicon Vertex Detectors (SVX,
SVX', SVXII) for Collider Detector at Fermilab (CDF) at the
Fermilab Tevatron have been fundamental tools for
heavy-flavor tagging via secondary vertex detection. The CDF
Run IIb Silicon Vertex Detector (SVXIIb) has been designed
to be a radiation-tolerant replacement for the currently
installed SVXII because SVXII was not expected to survive
the Tevatron luminosity anticipated for Run IIb. One major
change in the new design is the use of a single mechanical
and electrical element throughout the array. This element,
called a stave, carries six single-sided silicon sensors on
each side and is built using carbon fiber skins with a high
thermal conductivity on a foam core with a built-in cooling
channel. A Kapton bus cable carries power, data and control
signals underneath the silicon sensors on each side of the
stave. Sensors are read out in pairs via a ceramic hybrid
glued on one of the sensors and equipped with four SVX4
readout chips. This new design concept leads to a very
compact mechanical and electrical unit, allowing streamlined
production and ease of testing and installation. A
description of the design and mechanical performance of the
stave is given. Results on the electrical performance
obtained using prototype staves are also
presented.},
Doi = {10.1109/TNS.2004.835715},
Key = {fds308745}
}
@article{fds308748,
Author = {Collaboration, DAEACDF},
Title = {Central Pseudorapidity Gaps in Events with a Leading
Antiproton at the Fermilab Tevatron p-barp
Collider},
Journal = {Physical Review Letters},
Volume = {91},
Number = {1},
Pages = {011802},
Year = {2003},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.91.011802},
Abstract = {We report a measurement of the fraction of events with a
large pseudorapidity gap Delta eta within the pseudorapidity
region available to the proton dissociation products X in
p-bar+p-->p-bar+X. For a final state p-bar of fractional
momentum loss xi p-bar and 4-momentum transfer squared
tp-bar within 0.063 is found to be 0.246±0.001
(stat)±0.042 (syst) [0.184±0.001 (stat)±0.043 (syst)].
Our results are compared with gap fractions measured in
minimum bias p-barp collisions and with theoretical
expectations.},
Doi = {10.1103/physrevlett.91.011802},
Key = {fds308748}
}
@article{fds321223,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Centrality and rapidity dependence of inclusive jet
production in √sNN =5 .02 TeV proton–lead collisions
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {748},
Pages = {392-413},
Publisher = {Elsevier BV},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2015.07.023},
Abstract = {Measurements of the centrality and rapidity dependence of
inclusive jet production in sNN=5.02 TeV proton–lead
(p+Pb) collisions and the jet cross-section in s=2.76 TeV
proton–proton collisions are presented. These quantities
are measured in datasets corresponding to an integrated
luminosity of 27.8 nb−1 and 4.0 pb−1, respectively,
recorded with the ATLAS detector at the Large Hadron
Collider in 2013. The p+Pb collision centrality was
characterised using the total transverse energy measured in
the pseudorapidity interval −4.9 <η <−3.2 in the
direction of the lead beam. Results are presented for the
double-differential per-collision yields as a function of
jet rapidity and transverse momentum (pT) for minimum-bias
and centrality-selected p+Pb collisions, and are compared to
the jet rate from the geometric expectation. The total jet
yield in minimum-bias events is slightly enhanced above the
expectation in a pT-dependent manner but is consistent with
the expectation within uncertainties. The ratios of jet
spectra from different centrality selections show a strong
modification of jet production at all pT at forward
rapidities and for large pT at mid-rapidity, which manifests
as a suppression of the jet yield in central events and an
enhancement in peripheral events. These effects imply that
the factorisation between hard and soft processes is
violated at an unexpected level in proton–nucleus
collisions. Furthermore, the modifications at forward
rapidities are found to be a function of the total jet
energy only, implying that the violations may have a simple
dependence on the hard parton–parton kinematics.},
Doi = {10.1016/j.physletb.2015.07.023},
Key = {fds321223}
}
@article{fds315959,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Centrality, rapidity, and transverse momentum dependence of
isolated prompt photon production in lead-lead collisions at
sNN =2.76 TeV measured with the ATLAS detector},
Journal = {Physical Review C},
Volume = {93},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {March},
ISSN = {2469-9985},
url = {http://dx.doi.org/10.1103/PhysRevC.93.034914},
Abstract = {Prompt photon production in sNN=2.76-TeV Pb+Pb collisions
has been measured by the ATLAS experiment at the Large
Hadron Collider using data collected in 2011 with an
integrated luminosity of 0.14 nb-1. Inclusive photon yields,
scaled by the mean nuclear thickness function, are presented
as a function of collision centrality and transverse
momentum in two pseudorapidity intervals, |η|<1.37 and
1.52≤|η|<2.37. The scaled yields in the two
pseudorapidity intervals, as well as the ratios of the
forward yields to those at midrapidity, are compared to the
expectations from next-to-leading-order perturbative QCD
(pQCD) calculations. The measured cross sections agree well
with the predictions for proton-proton collisions within
statistical and systematic uncertainties. Both the yields
and the ratios are also compared to two other pQCD
calculations, one which uses the isospin content appropriate
to colliding lead nuclei and another which includes nuclear
modifications to the nucleon parton distribution
functions.},
Doi = {10.1103/PhysRevC.93.034914},
Key = {fds315959}
}
@article{fds308909,
Author = {al, FAE},
Title = {Charge asymmetry in w-boson decays produced in p(p)over-bar
collisions at root-s=1.8 tev},
Journal = {Phys. Rev. Lett.},
Volume = {74},
Number = {6},
Pages = {850-854},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevLett.74.850},
Abstract = {Charge asymmetry has been measured using 19 039 W decays
recorded by the Collider Detector at Fermilab during the
1992-93 run of the Tevatron Collider. The asymmetry is
sensitive to the ratio of d and u quark distributions to
x<0.01 at Q2MW2, where nonperturbative effects are minimal.
It is found that of the two current sets of parton
distributions, those of Martin, Roberts, and Stirling are
favored over the sets most recently produced by the CTEQ
Collaboration. The W asymmetry data provide stronger
constraints on du ratio than the recent measurements of
F2μnF2μp which are limited by uncertainties originating
from deuteron corrections. © 1995 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.74.850},
Key = {fds308909}
}
@article{fds308770,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson,
R and Dagenhart, D and D’Auria, S and DeJongh, F},
Title = {Charged jet evolution and the underlying event in
proton-antiproton collisions at 1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {65},
Number = {9},
Pages = {920021-9200222},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.65.092002},
Abstract = {The growth and development of “charged particle jets”
produced in proton-antiproton collisions at [Formula
Presented] are studied over a transverse momentum range from
[Formula Presented] [Formula Presented] to [Formula
Presented] [Formula Presented] A variety of leading (highest
transverse momentum) charged jet observables are compared
with the QCD Monte Carlo models HERWIG, ISAJET, and PYTHIA.
The models describe fairly well the multiplicity
distribution of charged particles within the leading charged
jet, the size of the leading charged jet, the radial
distribution of charged particles and transverse momentum
around the leading charged jet direction, and the momentum
distribution of charged particles within the leading charged
jet. The direction of the leading “charged particle jet”
in each event is used to define three regions of [Formula
Presented] space. The “toward” region contains the
leading “charged particle jet”, while the “away”
region, on the average, contains the away-side jet. The
“transverse” region is perpendicular to the plane of the
hard [Formula Presented]-to-[Formula Presented] scattering
and is very sensitive to the “underlying event”
component of the QCD Monte Carlo models. HERWIG, ISAJET, and
PYTHIA with their default parameters do not describe
correctly all the properties of the “transverse” region.
© 2002 The American Physical Society.},
Doi = {10.1103/PhysRevD.65.092002},
Key = {fds308770}
}
@article{fds321168,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel,
C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund,
OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan,
AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel,
O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio,
D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez,
SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El
Moursli, RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A},
Title = {Charged-particle distributions at low transverse momentum in
[Formula: see text] TeV pp interactions measured
with the ATLAS detector at the LHC.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {9},
Pages = {502},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4335-y},
Abstract = {Measurements of distributions of charged particles produced
in proton-proton collisions with a centre-of-mass energy of
13 TeV are presented. The data were recorded by the ATLAS
detector at the LHC and correspond to an integrated
luminosity of 151 [Formula: see text]. The particles are
required to have a transverse momentum greater than 100 MeV
and an absolute pseudorapidity less than 2.5. The
charged-particle multiplicity, its dependence on transverse
momentum and pseudorapidity and the dependence of the mean
transverse momentum on multiplicity are measured in events
containing at least two charged particles satisfying the
above kinematic criteria. The results are corrected for
detector effects and compared to the predictions from
several Monte Carlo event generators.},
Doi = {10.1140/epjc/s10052-016-4335-y},
Key = {fds321168}
}
@article{fds321189,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi,
S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier,
S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN},
Title = {Charged-particle distributions in pp interactions at
[Formula: see text] measured with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {7},
Pages = {403},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4203-9},
Abstract = {This paper presents measurements of distributions of charged
particles which are produced in proton-proton collisions at
a centre-of-mass energy of [Formula: see text] and recorded
by the ATLAS detector at the LHC. A special dataset recorded
in 2012 with a small number of interactions per beam
crossing (below 0.004) and corresponding to an integrated
luminosity of 160 [Formula: see text] was used. A
minimum-bias trigger was utilised to select a data sample of
more than 9 million collision events. The multiplicity,
pseudorapidity, and transverse momentum distributions of
charged particles are shown in different regions of
kinematics and charged-particle multiplicity, including
measurements of final states at high multiplicity. The
results are corrected for detector effects and are compared
to the predictions of various Monte Carlo event generator
models which simulate the full hadronic final
state.},
Doi = {10.1140/epjc/s10052-016-4203-9},
Key = {fds321189}
}
@article{fds315954,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Charged-particle distributions in √s=13 TeV pp
interactions measured with the ATLAS detector at the
LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {758},
Pages = {67-88},
Publisher = {Elsevier BV},
Year = {2016},
Month = {July},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2016.04.050},
Abstract = {Charged-particle distributions are measured in
proton–proton collisions at a centre-of-mass energy of 13
TeV, using a data sample of nearly 9 million events,
corresponding to an integrated luminosity of 170 μb−1,
recorded by the ATLAS detector during a special Large Hadron
Collider fill. The charged-particle multiplicity, its
dependence on transverse momentum and pseudorapidity and the
dependence of the mean transverse momentum on the
charged-particle multiplicity are presented. The
measurements are performed with charged particles with
transverse momentum greater than 500 MeV and absolute
pseudorapidity less than 2.5, in events with at least one
charged particle satisfying these kinematic requirements.
Additional measurements in a reduced phase space with
absolute pseudorapidity less than 0.8 are also presented, in
order to compare with other experiments. The results are
corrected for detector effects, presented as particle-level
distributions and are compared to the predictions of various
Monte Carlo event generators.},
Doi = {10.1016/j.physletb.2016.04.050},
Key = {fds315954}
}
@article{fds308785,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and Brink, SV and Bromberg, C and Brozovic, M and Brubaker,
E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera,
S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan,
AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung,
YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin,
T and Dittmann, JR and Dominguez, A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Erbacher, R and Errede, D and Errede, S and Fan, Q and Feild,
RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman,
J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov, I and Goshaw,
AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Lee, AM and Lee, K and Leone, S and Lewis, JD and Lindgren,
M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos,
A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Roy,
A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg,
D and Sanchez, C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding,
J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda,
H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
F and Vaiciulis, T and Valls, J and Vejcik, S and Velev, G and Veramendi,
G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters,
D and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Charged-particle multiplicity p p̄ collisions at √s = 1.8
TeV},
Journal = {Physical Review Letters},
Volume = {87},
Number = {21},
Pages = {2118041-2118046},
Year = {2001},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.87.211804},
Abstract = {The mean charged-particle multiplicity of jets in dijet
events with dijet masses were analyzed using collider
detectors. The jet energy and direction were measured in the
central lead-scintillator electromagnetic (CEM) and
iron-scintillator hadronic (CHA) calorimeters. It is shown
that the fraction of gluon jets decreases to 23%-26% at 630
GeV/c2 from 61%-63% of all jets at 80 GeV/c2.},
Doi = {10.1103/physrevlett.87.211804},
Key = {fds308785}
}
@article{fds308396,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Asman, B and Atkins, S and Atramentov, O and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barreto, J and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Belanger-Champagne, C and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bezzubov, VA and Bhatia, S and Bhatnagar, V and Bhatti, A and Bhat, PC and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Brooijmans, G and Bross, A and Brown, D and Brown, J and Brucken, E and Bu,
XB},
Title = {Combination of CDF and D0 measurements of the W boson
helicity in top quark decays},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.85.071106},
Abstract = {We report the combination of recent measurements of the
helicity of the W boson from top quark decay by the CDF and
D0 collaborations, based on data samples corresponding to
integrated luminosities of 2.7-5.4fb -1 of pp̄ collisions
collected during Run II of the Fermilab Tevatron collider.
Combining measurements that simultaneously determine the
fractions of W bosons with longitudinal (f 0) and
right-handed (f +) helicities, we find f
0=0.722±0.081[±0.062(stat)±0.052(syst)] and f
+=-0.033±0.046[±0.034(stat)±0.031(syst)]. Combining
measurements where one of the helicity fractions is fixed to
the value expected in the standard model, we find f
0=0.682±0. 057[±0.035(stat)±0.046(syst)] for fixed f +
and f +=-0.015±0.035[±0.018(stat)±0.030(syst)] for fixed
f 0. The results are consistent with standard model
expectations. © 2012 American Physical Society.},
Doi = {10.1103/PhysRevD.85.071106},
Key = {fds308396}
}
@article{fds308734,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Acosta, D and Adams, DL and Adams, M and Affolder, T and Ahmed, SN and Akimoto, H and Akopian, A and Albrow, MG and Alexeev, GD and Alton, A and Alves, GA and Amaral, P and Ambrose, D and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arnoud, Y and Arisawa, T and Artikov, A and Asakawa, T and Avila, C and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Babintsev, VV and Babukhadia, L and Bacchetta, N and Bachacou, H and Bacon, TC and Baden,
A and Badgett, W and Baffioni, S and Bailey, MW and Bailey, S and Baldin,
B and Balm, PW and Banerjee, S and Barbaro, P and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Baroiant,
S and Barone, M and Barreto, J and Bartlett, JF and Bassler, U and Bauer,
D and Bauer, G and Bean, A and Beaudette, F and Bedeschi, F and Behari, S and Begel, M and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Belyaev, A and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Beri, SB and Bernardi, G and Bertram, I and Berryhill, J and Besson, A and Beuselinck, R and Bevensee, B and Bezzubov, VA and Bhat,
PC and Bhatnagar, V and Bhattacharjee, M and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blazey, G and Blekman, F and Blessing, S and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Boehnlein, A and Bojko,
NI},
Title = {Combination of CDF and D0 results on the [Formula Presented]
boson mass and width},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {70},
Number = {9},
Pages = {092008-1-092008-17},
Publisher = {American Physical Society (APS)},
Year = {2004},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.70.092008},
Abstract = {The results based on 1992–95 data (Run 1) from the CDF and
D0 experiments on the measurements of the [Formula
Presented] boson mass and width are presented, along with
the combined results. We report a Tevatron collider average
[Formula Presented]. We also report the Tevatron collider
average of the directly measured [Formula Presented] boson
width [Formula Presented]. We describe a new joint analysis
of the direct [Formula Presented] mass and width
measurements. Assuming the validity of the standard model,
we combine the directly measured [Formula Presented] boson
width with the width extracted from the ratio of [Formula
Presented] and [Formula Presented] boson leptonic partial
cross sections. This combined result for the Tevatron is
[Formula Presented]. Finally, we use the measurements of the
direct total [Formula Presented] width and the leptonic
branching ratio to extract the leptonic partial width
[Formula Presented]. © 2004 The American Physical
Society.},
Doi = {10.1103/PhysRevD.70.092008},
Key = {fds308734}
}
@article{fds308312,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Beecher, D and Begalli, M and Behari, S and Bellantoni,
L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon,
M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti,
A and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Boudreau, J and Boveia,
A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg,
C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd,
HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P},
Title = {Combination of CDF and D0 W-Boson mass measurements},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {5},
Pages = {052018},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.88.052018},
Abstract = {We summarize and combine direct measurements of the mass of
the W boson in √s=1.96 TeV proton-antiproton collision
data collected by CDF and D0 experiments at the Fermilab
Tevatron Collider. Earlier measurements from CDF and D0 are
combined with the two latest, more precise measurements: a
CDF measurement in the electron and muon channels using data
corresponding to 2.2 fb-1 of integrated luminosity, and a D0
measurement in the electron channel using data corresponding
to 4.3 fb-1 of integrated luminosity. The resulting Tevatron
average for the mass of the W boson is M W=80387±16 MeV.
Including measurements obtained in electron-positron
collisions at LEP yields the most precise value of M
W=80385±15 MeV. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.052018},
Key = {fds308312}
}
@article{fds308277,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu,
A},
Title = {Combination of measurements of the top-quark pair production
cross section from the Tevatron Collider},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.89.072001},
Abstract = {We combine six measurements of the inclusive top-quark pair
(tt̄) production cross section (σtt̄) from data collected
with the CDF and D0 detectors at the Fermilab Tevatron with
proton-antiproton collisions at s=1.96TeV. The data
correspond to integrated luminosities of up to 8.8fb-1. We
obtain a value of σtt̄=7.60±0.41pb for a top-quark mass
of mt=172.5GeV. The contributions to the uncertainty are
0.20 pb from statistical sources, 0.29 pb from systematic
sources, and 0.21 pb from the uncertainty on the integrated
luminosity. The result is in good agreement with the
standard model expectation of 7.35-0.33+0.28pb at
next-to-next-to-leading order and next-to-next-to leading
logarithms in perturbative QCD. © 2014 American Physical
Society.},
Doi = {10.1103/PhysRevD.89.072001},
Key = {fds308277}
}
@article{fds375932,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH},
Title = {Combination of searches for invisible decays of the Higgs
boson using 139 fb−1 of proton-proton collision
data at s=13 TeV collected with the ATLAS
experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {842},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137963},
Abstract = {Many extensions of the Standard Model predict the production
of dark matter particles at the LHC. Sufficiently light dark
matter particles may be produced in decays of the Higgs
boson that would appear invisible to the detector. This
Letter presents a statistical combination of searches for
H→invisible decays where multiple production modes of the
Standard Model Higgs boson are considered. These searches
are performed with the ATLAS detector using 139 fb−1 of
proton–proton collisions at a centre–of–mass energy of
[Formula presented] at the LHC. In combination with the
results at [Formula presented] and [Formula presented], an
upper limit on the H→invisible branching ratio of 0.107
(0.077) at the 95% confidence level is observed (expected).
These results are also interpreted in the context of models
where the 125 GeV Higgs boson acts as a portal to dark
matter, and limits are set on the scattering cross-section
of weakly interacting massive particles and
nucleons.},
Doi = {10.1016/j.physletb.2023.137963},
Key = {fds375932}
}
@article{fds308315,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Combination of searches for the Higgs boson using the full
CDF data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.88.052013},
Abstract = {We present a combination of searches for the standard model
Higgs boson using the full CDF run II data set, which
corresponds to an integrated luminosity of 9.45-10.0 fb-1
collected from √s=1.96 TeV pp̄ collisions at the Fermilab
Tevatron. The searches consider Higgs boson production from
gluon-gluon fusion, vector-boson fusion, and associated
production with either a W or Z boson or a tt̄ pair.
Depending on the production mode, Higgs boson decays to
W+W-, ZZ, bb̄, τ+τ-, and γγ are examined. We search for
a Higgs boson with masses (mH) in the range 90-200 GeV/c2.
In the absence of a signal, we expect based on combined
search sensitivity to exclude at the 95% credibility level
the mass regions 90<mH<94 GeV/c2, 96<mH<106 GeV/c2, and
153<mH<175 GeV/c2. The observed exclusion regions are
90<mH<102 GeV/c2 and 149<mH<172 GeV/c2. A moderate excess of
signal-like events relative to the background expectation at
the level of 2.0 standard deviations is present in the data
for the mH=125 GeV/c2 search hypothesis. We also present
interpretations of the data within the context of a
fermiophobic model and an alternative standard model
incorporating a fourth generation of fermions. Finally, for
the hypothesis of a new particle with mass 125 GeV/c2, we
constrain the coupling strengths of the new particle to W±
bosons, Z bosons, and fermions. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.052013},
Key = {fds308315}
}
@article{fds308485,
Author = {Aaltonen, and T, and others},
Title = {Combination of Tevatron searches for the standard model
Higgs boson in the $W^+W^-$ decay mode},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {6},
Pages = {061802},
Year = {2010},
url = {http://arXiv.org/abs/1001.4162},
Abstract = {http://arxiv.org/abs/1001.4162},
Doi = {10.1103/PhysRevLett.104.061802},
Key = {fds308485}
}
@article{fds308385,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori,
L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett,
K},
Title = {Combination of the top-quark mass measurements from the
Tevatron collider},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {9},
Pages = {092003},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.86.092003},
Abstract = {The top quark is the heaviest known elementary particle,
with a mass about 40 times larger than the mass of its
isospin partner, the bottom quark. It decays almost 100% of
the time to a W boson and a bottom quark. Using top-antitop
pairs at the Tevatron proton-antiproton collider, the CDF
and D0 Collaborations have measured the top quark's mass in
different final states for integrated luminosities of up to
5.8fb-1. This paper reports on a combination of these
measurements that results in a more precise value of the
mass than any individual decay channel can provide. It
describes the treatment of the systematic uncertainties and
their correlations. The mass value determined is
173.18±0.56(stat)±0.75(syst)GeV or 173.18±0.94GeV, which
has a precision of ±0.54%, making this the most precise
determination of the top-quark mass. © 2012 American
Physical Society.},
Doi = {10.1103/PhysRevD.86.092003},
Key = {fds308385}
}
@article{fds308617,
Author = {Kruse, MC and group, EAWTTEVNPHW},
Title = {Combined CDF and D0 Upper Limits on Standard Model Higgs
Boson Production at High Mass (155-200-GeV/c^2) with 3 fb^-1
of data},
Journal = {e-Print: arXiv:0808.0534},
Year = {2008},
url = {http://arviv.org/pdf/0808.0534},
Key = {fds308617}
}
@article{fds375888,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arbiol
Val, SJ and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Artoni,
G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal,
D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Baer, TM and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barel, MZ and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beaucamp, JY and Beauchemin, PH and Becherer, F and Bechtle, P and Beck,
HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berrocal Guardia and A and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhalla, NK and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov,
VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borissov, G and Bortoletto, D and Boscherini,
D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton,
D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost,
E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
PA and Brüers, B and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlotto, JI and Carlson,
BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos,
F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM},
Title = {Combined Measurement of the Higgs Boson Mass from the
H→γγ and H→ZZ^{*}→4ℓ Decay Channels with the ATLAS
Detector Using sqrt[s]=7, 8, and 13 TeV pp Collision
Data.},
Journal = {Physical review letters},
Volume = {131},
Number = {25},
Pages = {251802},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.131.251802},
Abstract = {A measurement of the mass of the Higgs boson combining the
H→ZZ^{*}→4ℓ and H→γγ decay channels is presented.
The result is based on 140 fb^{-1} of proton-proton
collision data collected by the ATLAS detector during LHC
run 2 at a center-of-mass energy of 13 TeV combined with
the run 1 ATLAS mass measurement, performed at
center-of-mass energies of 7 and 8 TeV, yielding a Higgs
boson mass of 125.11±0.09(stat)±0.06(syst)=125.11±0.11 GeV.
This corresponds to a 0.09% precision achieved on this
fundamental parameter of the Standard Model of particle
physics.},
Doi = {10.1103/physrevlett.131.251802},
Key = {fds375888}
}
@article{fds321251,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
Title = {Combined Measurement of the Higgs Boson Mass in pp
Collisions at sqrt[s]=7 and 8 TeV with the ATLAS and CMS
Experiments.},
Journal = {Physical review letters},
Volume = {114},
Number = {19},
Pages = {191803},
Year = {2015},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.114.191803},
Abstract = {A measurement of the Higgs boson mass is presented based on
the combined data samples of the ATLAS and CMS experiments
at the CERN LHC in the H→γγ and H→ZZ→4ℓ decay
channels. The results are obtained from a simultaneous fit
to the reconstructed invariant mass peaks in the two
channels and for the two experiments. The measured masses
from the individual channels and the two experiments are
found to be consistent among themselves. The combined
measured mass of the Higgs boson is m_{H}=125.09±0.21
(stat)±0.11 (syst) GeV.},
Doi = {10.1103/physrevlett.114.191803},
Key = {fds321251}
}
@article{fds308614,
Author = {al, EAE},
Title = {Combined performance tests before installation of the ATLAS
Semiconductor and Transition Radiation Tracking
Detectors},
Journal = {Jinst 3 P08003},
Volume = {3},
Number = {8},
Pages = {P08003-P08003},
Publisher = {IOP Publishing},
Year = {2008},
url = {http://dx.doi.org/10.1088/1748-0221/3/08/P08003},
Abstract = {The ATLAS (A Toroidal LHC ApparatuS) Inner Detector provides
charged particle tracking in the centre of the ATLAS
experiment at the Large Hadron Collider (LHC). The Inner
Detector consists of three subdetectors: the Pixel Detector,
the Semiconductor Tracker (SCT), and the Transition
Radiation Tracker (TRT). This paper summarizes the tests
that were carried out at the final stage of SCT+TRT
integration prior to their installation in ATLAS. The
combined operation and performance of the SCT and TRT barrel
and endcap detectors was investigated through a series of
noise tests, and by recording the tracks of cosmic rays.
This was a crucial test of hardware and software of the
combined tracker detector systems. The results of noise and
cross-talk tests on the SCT and TRT in their final assembled
configuration, using final readout and supply hardware and
software, are reported. The reconstruction and analysis of
the recorded cosmic tracks allowed testing of the offline
analysis chain and verification of basic tracker performance
parameters, such as efficiency and spatial resolution, in
combined operation before installation. © 2008 IOP
Publishing Ltd. and SISSA.},
Doi = {10.1088/1748-0221/3/08/P08003},
Key = {fds308614}
}
@article{fds321372,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
ME and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci,
A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington,
S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeans, DT and Jeon, EJ and Jindariani, S and Jones,
M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi,
A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Tipton, P and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund,
AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Combined search for the standard model Higgs boson decaying
to a bb pair using the full CDF data set.},
Journal = {Physical review letters},
Volume = {109},
Number = {11},
Pages = {111802},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.109.111802},
Abstract = {We combine the results of searches for the standard model
(SM) Higgs boson based on the full CDF Run II data set
obtained from sqrt[s]=1.96 TeV pp collisions at the
Fermilab Tevatron corresponding to an integrated luminosity
of 9.45 fb(-1). The searches are conducted for Higgs
bosons that are produced in association with a W or Z boson,
have masses in the range 90-150 GeV/c(2), and decay
into bb pairs. An excess of data is present that is
inconsistent with the background prediction at the level of
2.5 standard deviations (the most significant local excess
is 2.7 standard deviations).},
Doi = {10.1103/physrevlett.109.111802},
Key = {fds321372}
}
@article{fds308488,
Author = {Aaltonen, and T, and others},
Title = {Combined Tevatron upper limit on $gg\rightarrow{}H\rightarrow{}W^{+}W^{-}$
and constraints on the Higgs boson mass in fourth-generation
fermion models},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {1},
Pages = {011102},
Publisher = {American Physical Society},
Year = {2010},
Month = {July},
url = {http://inspirehep.net/record/855342},
Abstract = {We combine results from searches by the CDF and D0
collaborations for a standard model Higgs boson (H) in the
process gg→H→W+W - in pp̄ collisions at the Fermilab
Tevatron Collider at √s=1.96TeV. With 4.8fb-1 of
integrated luminosity analyzed at CDF and 5.4fb-1 at D0, the
95% confidence level upper limit on σ(gg→H)×B(H→W+W-)
is 1.75 pb at mH=120GeV, 0.38 pb at mH=165GeV, and 0.83 pb
at mH=200GeV. Assuming the presence of a fourth sequential
generation of fermions with large masses, we exclude at the
95% confidence level a standard-model-like Higgs boson with
a mass between 131 and 204 GeV. © 2010 The American
Physical Society.},
Doi = {10.1103/PhysRevD.82.011102},
Key = {fds308488}
}
@article{fds308511,
Author = {Bethke, S and Aaltonen, T and Adelman, J and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Antos, J and Apollinari,
G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Azzurri, P and Badgett, W and Barnett, BA and Bartsch, V and Beecher, D and Behari, S and Bellettini, G and Benjamin, D and Bisello, D and Bizjak,
I and Blocker, C and Blumenfeld, B and Bocci, A and Boisvert, V and Bolla,
G and Bortoletto, D and Boudreau, J and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Canelli, F and Carls,
B and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli,
D and Chou, JP and Chung, K and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and Dell'Orso, M and Demortier,
L and Deng, J and Deninno, M and di Giovanni, GP and Di Ruzza and B and Dittmann, JR and Donati, S and Donini, J and Dorigo, T and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fedorko,
WT},
Title = {Comments and Reply on: "Study of multi-muon events produced
in pp̄ interactions at √s = 1.96 TeV"; T. Aaltonen et al.
(The CDF collaboration)},
Journal = {European Physical Journal C},
Volume = {68},
Number = {1},
Pages = {119-123},
Publisher = {Springer Nature},
Year = {2010},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-010-1337-z},
Abstract = {The European Physical Journal C-Particles and
Fields-publishes scientific manuscripts of relevance to the
scientific community following careful and strict peer
reviewing and, whenever appropriate and necessary, through
discussion with the authors, so as to optimise scientific
content and style of presentation prior to publication. In
some cases significant disagreement between authors and
referees (and/or editors) of the journal cannot be resolved
despite all efforts and best of intentions. While the
journal-notwithstanding any appeals-retains the right to
reject such manuscripts, the editors of this journal may
decide, in cases deemed of exceptional interest and
potential significance for the field, to accept the
manuscript for publication, to amend it by "comments" of the
editor(s) in charge and, if appropriate, by a "reply" of the
authors of the commented manuscript. The present comment is
on "Study of multi-muon events produced in pp̄ interactions
at √ = 1.96 TeV"; T. Aaltonen et al. (The CDF
Collaboration, Eur. Phys. J. C, 2010, doi:10.1140/epjc/s10052-010-1336-0.
© 2010 The Author(s).},
Doi = {10.1140/epjc/s10052-010-1337-z},
Key = {fds308511}
}
@article{fds375890,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Comparison of inclusive and photon-tagged jet suppression in
5.02 TeV Pb+Pb collisions with ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {846},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138154},
Abstract = {Parton energy loss in the quark–gluon plasma (QGP) is
studied with a measurement of photon-tagged jet production
in 1.7 nb−1 of Pb+Pb data and 260 pb−1 of pp data, both
at sNN=5.02 TeV, with the ATLAS detector. The process pp
→γ+jet+X and its analogue in Pb+Pb collisions is measured
in events containing an isolated photon with transverse
momentum (pT) above 50 GeV and reported as a function of jet
pT. This selection results in a sample of jets with a
steeply falling pT distribution that are mostly initiated by
the showering of quarks. The pp and Pb+Pb measurements are
used to report the nuclear modification factor, RAA, and the
fractional energy loss, Sloss, for photon-tagged jets. In
addition, the results are compared with the analogous ones
for inclusive jets, which have a significantly smaller
quark-initiated fraction. The RAA and Sloss values are found
to be significantly different between those for
photon-tagged jets and inclusive jets, demonstrating that
energy loss in the QGP is sensitive to the colour-charge of
the initiating parton. The results are also compared with a
variety of theoretical models of colour-charge-dependent
energy loss.},
Doi = {10.1016/j.physletb.2023.138154},
Key = {fds375890}
}
@article{fds331228,
Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera,
S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan,
AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Colijn, AP and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R},
Title = {Comparison of the isolated direct photon cross sections in
[Formula Presented] collisions at [Formula Presented] and
[Formula Presented]},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {65},
Number = {11},
Pages = {10},
Publisher = {American Physical Society (APS)},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.65.112003},
Abstract = {We have measured the cross sections (Formula presented) for
production of isolated direct photons in (Formula presented)
collisions at two different center-of-mass energies, 1.8 TeV
and 0.63 TeV, using the Collider Detector at Fermilab. The
normalization of both data sets agrees with the predictions
of quantum chromodynamics for a photon transverse momentum
(Formula presented) of 25 GeV/c, but the shapes versus
photon (Formula presented) do not. These shape differences
lead to a significant disagreement in the ratio of cross
sections in the scaling variable (Formula presented) This
disagreement in the (Formula presented) ratio is difficult
to explain with conventional theoretical uncertainties such
as scale dependence and parton distribution
parametrizations. © 2002 The American Physical
Society.},
Doi = {10.1103/PhysRevD.65.112003},
Key = {fds331228}
}
@article{fds340917,
Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
J and Culbertson, R and Dagenhart, D and D'Auria, S and Barbaro, PD and Cecco, SD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi,
C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Farrington, S and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Flores-Castillo, LR and Foster, GW and Franklin, M and Friedman, J and Furic, I and Gallinaro, M and Garfinkel, AF and Gay, C and Gerdes, DW and Gerstein, E and Giagu, S and Giannetti, P and Giolo, K and Giordani, M and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn,
SR and Halkiadakis, E and Handler, R and Happacher, F and Hara, K and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
J and Hennecke, M and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hou, S and Huffman, BT and Hughes, R and Huston, J and Incandela, J and Introzzi, G and Iori, M and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jones, M and Kamon, T and Kang, J and Unel, MK and Kartal, S and Kasha, H and Kato, Y and Kennedy, RD and Kephart, R and Kilminster, B and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, TH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Koehn,
P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lami, S and Lammel, S and Lancaster, J and Lancaster,
M and Lander, R and Lannon, K and Lath, A and Latino, G and LeCompte, T and Le, Y and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu,
T and Lockyer, NS and Loginov, A and Loreti, M and Lucchesi, D and Lukens,
P and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Mangano, M and Mariotti, M and Martin, A and Martin, M and Martin, V and Martínez, M and Mazzanti, P and McFarland,
KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, JS and Miller, R and Miscetti, S and Mitselmakher, G and Moggi, N and Moore, R and Moulik, T and Mukherjee, A and Mulhearn, M and Muller, T and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napora, R and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Niell, F and Nigmanov, T and Nodulman, L and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Pompoš,
A and Pondrom, L and Pope, G and Poukhov, O and Pratt, T and Prokoshin, F and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine,
A and Ratnikov, F and Ray, H and Reichold, A and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Ryan, D and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti, A and Sill, A and Sinervo, P and Slaughter, AJ and Sliwa, K and Snider, FD and Snihur, R and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Stefanini, A and Strologas, J and Stuart, D and Sukhanov, A and Sumorok,
K and Suzuki, T and Takashima, R and Takikawa, K and Tanaka, M and Tecchio,
M and Teng, PK and Terashi, K and Tesarek, RJ and Tether, S and Thorn, J and Thomas, TL and Thompson, AS and Thomson, E and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tonelli, D and Tönnesmann, M and Toyoda,
H and Trischuk, W and Tseng, J and Tsybychev, D and Turini, N and Ukegawa,
F and Unverhau, T and Vaiciulis, T and Varganov, A and Vataga, E and III,
SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Wagner, RG and Wagner, RL and Wagner, W and Wan, Z and Wang, C and Wang, MJ and Wang, SM and Ward, B and Waschke, S and Waters, D and Watts, T and Weber, M and III, WCW and Whitehouse, B and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
BL and Wolbers, S and Wolter, M and Worm, S and Wu, X and Würthwein, F and Yang, UK and Yao, W and Yeh, GP and Yi, K and Yoh, J and Yoshida, T and Yu, I and Yu, S and Yun, JC and Zanello, L and Zanetti, A and Zetti, F and Zucchelli,
S},
Title = {Comparison of three-jet events in pp̄ collisions at √s =
1.8 TeV to predictions from a next-to-leading order QCD
calculation},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {3},
Pages = {032002-1-032002-12},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.032002},
Abstract = {The properties of three-jet events with total transverse
energy greater than 320 GeV and individual jet energy
greater than 20 GeV have been analyzed and compared to
absolute predictions from a next-to-leading order (NLO)
perturbative QCD calculation. These data, of integrated
luminosity 86 pb -1, were recorded by the CDF Experiment for
pp collisions at √s = 1.8 TeV This study tests a model of
higher order QCD processes that result in gluon emission and
may give some indication of the magnitude of the
contribution of processes higher than NLO. The total cross
section is measured to be 466 ± 3(stat.)-70+207(syst.) pb.
The differential cross section is furthermore measured for
all kinematically accessible regions of the Dalitz plane,
including those for which the theoretical prediction is
unreliable. While the measured cross section is consistent
with the theoretical prediction in magnitude, the two differ
somewhat in shape in the Dalitz plane. © 2005 The American
Physical Society.},
Doi = {10.1103/PhysRevD.71.032002},
Key = {fds340917}
}
@article{fds321308,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Comprehensive measurements of t-channel single top-quark
production cross sections at √s=7 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.90.112006},
Abstract = {This article presents measurements of the t-channel single
top-quark (t) and top-antiquark (t¯) total production cross
sections σ(tq) and σ(t¯q), their ratio
Rt=σ(tq)/σ(t¯q), and a measurement of the inclusive
production cross section σ(tq+t¯q) in proton-proton
collisions at √s=7 TeV at the LHC. Differential cross
sections for the tq and t¯q processes are measured as a
function of the transverse momentum and the absolute value
of the rapidity of t and t¯, respectively. The analyzed
data set was recorded with the ATLAS detector and
corresponds to an integrated luminosity of 4.59 fb-1.
Selected events contain one charged lepton, large missing
transverse momentum, and two or three jets. The cross
sections are measured by performing a binned
maximum-likelihood fit to the output distributions of neural
networks. The resulting measurements are
σ(tq)=46±1(stat)±6(syst) pb, σ(t¯q)=23±1(stat)±3(syst)
pb, Rt=2.04±0.13(stat)±0.12(syst), and
σ(tq+t¯q)=68±2(stat)±8(syst) pb, consistent with the
Standard Model expectation. The uncertainty on the measured
cross sections is dominated by systematic uncertainties,
while the uncertainty on Rt is mainly statistical. Using the
ratio of σ(tq+t¯q) to its theoretical prediction, and
assuming that the top-quark-related CKM matrix elements obey
the relation |Vtb||Vts|,|Vtd|, we determine
|Vtb|=1.02±0.07.},
Doi = {10.1103/PhysRevD.90.112006},
Key = {fds321308}
}
@article{fds365366,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alison, J and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
Bella, L and Aranzabal, N and Araujo Ferraz and V and Pereira, RA and Arcangeletti, C and Arce, ATH},
Title = {Configuration and performance of the ATLAS b-jet triggers in
Run 2},
Journal = {European Physical Journal C},
Volume = {81},
Number = {12},
Year = {2021},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09775-5},
Abstract = {Several improvements to the ATLAS triggers used to identify
jets containing b-hadrons (b-jets) were implemented for
data-taking during Run 2 of the Large Hadron Collider from
2016 to 2018. These changes include reconfiguring the b-jet
trigger software to improve primary-vertex finding and allow
more stable running in conditions with high pile-up, and the
implementation of the functionality needed to run
sophisticated taggers used by the offline reconstruction in
an online environment. These improvements yielded an order
of magnitude better light-flavour jet rejection for the same
b-jet identification efficiency compared to the performance
in Run 1 (2011–2012). The efficiency to identify b-jets
in the trigger, and the conditional efficiency for b-jets
that satisfy offline b-tagging requirements to pass the
trigger are also measured. Correction factors are derived to
calibrate the b-tagging efficiency in simulation to match
that observed in data. The associated systematic
uncertainties are substantially smaller than in previous
measurements. In addition, b-jet triggers were operated for
the first time during heavy-ion data-taking, using dedicated
triggers that were developed to identify semileptonic
b-hadron decays by selecting events with geometrically
overlapping muons and jets.},
Doi = {10.1140/epjc/s10052-021-09775-5},
Key = {fds365366}
}
@article{fds365354,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C and Arce, ATH and Arguin, JF},
Title = {Constraints on Higgs boson properties using
WW∗(→ eνμν) jj production in
36.1fb-1 of √s=13 TeV pp collisions with the
ATLAS detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {7},
Year = {2022},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10366-1},
Abstract = {This article presents the results of two studies of Higgs
boson properties using the WW∗(→ eνμν) jj final
state, based on a dataset corresponding to 36.1 fb - 1 of
s=13 TeV proton–proton collisions recorded by the ATLAS
experiment at the Large Hadron Collider. The first study
targets Higgs boson production via gluon–gluon fusion and
constrains the CP properties of the effective Higgs–gluon
interaction. Using angular distributions and the overall
rate, a value of tan (α) = 0.0 ± 0.4 (stat.) ± 0.3
(syst.) is obtained for the tangent of the mixing angle for
CP-even and CP-odd contributions. The second study exploits
the vector-boson fusion production mechanism to probe the
Higgs boson couplings to longitudinally and transversely
polarised W and Z bosons in both the production and the
decay of the Higgs boson; these couplings have not been
directly constrained previously. The polarisation-dependent
coupling-strength scale factors are defined as the ratios of
the measured polarisation-dependent coupling strengths to
those predicted by the Standard Model, and are determined
using rate and kinematic information to be
aL=0.91-0.18+0.10(stat.)-0.17+0.09(syst.) and aT= 1.2 ± 0.4
(stat.)-0.3+0.2(syst.). These coupling strengths are
translated into pseudo-observables, resulting in
κVV=0.91-0.18+0.10(stat.)-0.17+0.09(syst.) and
ϵVV=0.13-0.20+0.28 (stat.)-0.10+0.08(syst.). All results
are consistent with the Standard Model predictions.},
Doi = {10.1140/epjc/s10052-022-10366-1},
Key = {fds365354}
}
@article{fds321257,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo,
N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Galloni, C and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn,
SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes,
RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori,
M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
L and Margaroli, F and Marino, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and (CDF
Collaboration)},
Title = {Constraints on models of the Higgs boson with exotic spin
and parity using decays to bottom-antibottom quarks in the
full CDF data set.},
Journal = {Physical review letters},
Volume = {114},
Number = {14},
Pages = {141802},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.114.141802},
Abstract = {A search for particles with the same mass and couplings as
those of the standard model Higgs boson but different spin
and parity quantum numbers is presented. We test two
specific alternative Higgs boson hypotheses: a pseudoscalar
Higgs boson with spin-parity J^{P}=0^{-} and a gravitonlike
Higgs boson with J^{P}=2^{+}, assuming for both a mass of
125 GeV/c^{2}. We search for these exotic states
produced in association with a vector boson and decaying
into a bottom-antibottom quark pair. The vector boson is
reconstructed through its decay into an electron or muon
pair, or an electron or muon and a neutrino, or it is
inferred from an imbalance in total transverse momentum. We
use expected kinematic differences between events containing
exotic Higgs bosons and those containing standard model
Higgs bosons. The data were collected by the CDF experiment
at the Tevatron proton-antiproton collider, operating at a
center-of-mass energy of sqrt[s]=1.96 TeV, and
correspond to an integrated luminosity of 9.45 fb^{-1}.
We exclude deviations from the predictions of the standard
model with a Higgs boson of mass 125 GeV/c^{2} at the
level of 5 standard deviations, assuming signal strengths
for exotic boson production equal to the prediction for the
standard model Higgs boson, and set upper limits of
approximately 30% relative to the standard model rate on the
possible rate of production of each exotic
state.},
Doi = {10.1103/physrevlett.114.141802},
Key = {fds321257}
}
@article{fds375944,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Constraints on spin-0 dark matter mediators and invisible
Higgs decays using ATLAS 13 TeV pp collision data with two
top quarks and missing transverse momentum in the final
state},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11477-z},
Abstract = {This paper presents a statistical combination of searches
targeting final states with two top quarks and invisible
particles, characterised by the presence of zero, one or two
leptons, at least one jet originating from a b-quark and
missing transverse momentum. The analyses are searches for
phenomena beyond the Standard Model consistent with the
direct production of dark matter in pp collisions at the
LHC, using 139 fb - 1 of data collected with the ATLAS
detector at a centre-of-mass energy of 13 TeV. The results
are interpreted in terms of simplified dark matter models
with a spin-0 scalar or pseudoscalar mediator particle. In
addition, the results are interpreted in terms of upper
limits on the Higgs boson invisible branching ratio, where
the Higgs boson is produced according to the Standard Model
in association with a pair of top quarks. For scalar
(pseudoscalar) dark matter models, with all couplings set to
unity, the statistical combination extends the mass range
excluded by the best of the individual channels by
50 (25) GeV, excluding mediator masses up to 370 GeV. In
addition, the statistical combination improves the expected
coupling exclusion reach by 14% (24%), assuming a scalar
(pseudoscalar) mediator mass of 10 GeV. An upper limit on
the Higgs boson invisible branching ratio of 0.38
(0.30-0.09+0.13) is observed (expected) at 95% confidence
level.},
Doi = {10.1140/epjc/s10052-023-11477-z},
Key = {fds375944}
}
@article{fds375916,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Constraints on the Higgs boson self-coupling from single-
and double-Higgs production with the ATLAS detector using pp
collisions at s=13 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137745},
Abstract = {Constraints on the Higgs boson self-coupling are set by
combining double-Higgs boson analyses in the bb¯bb¯,
bb¯τ+τ− and bb¯γγ decay channels with single-Higgs
boson analyses targeting the γγ, ZZ⁎, WW⁎, τ+τ−
and bb¯ decay channels. The data used in these analyses
were recorded by the ATLAS detector at the LHC in
proton–proton collisions at s=13 TeV and correspond to an
integrated luminosity of 126–139 fb−1. The combination
of the double-Higgs analyses sets an upper limit of μHH<2.4
at 95% confidence level on the double-Higgs production
cross-section normalised to its Standard Model prediction.
Combining the single-Higgs and double-Higgs analyses, with
the assumption that new physics affects only the Higgs boson
self-coupling (λHHH), values outside the interval
−0.4<κλ=(λHHH/λHHHSM)<6.3 are excluded at 95%
confidence level. The combined single-Higgs and double-Higgs
analyses provide results with fewer assumptions, by adding
in the fit more coupling modifiers introduced to account for
the Higgs boson interactions with the other Standard Model
particles. In this relaxed scenario, the constraint becomes
−1.4<κλ<6.1 at 95% CL.},
Doi = {10.1016/j.physletb.2023.137745},
Key = {fds375916}
}
@article{fds321300,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Piqueras, DÁ and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Constraints on the off-shell Higgs boson signal strength in
the high-mass ZZ and WW final states with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {335},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3542-2},
Abstract = {Measurements of the <i>ZZ</i> and <i>WW</i> final states in
the mass range above the [Formula: see text] and [Formula:
see text] thresholds provide a unique opportunity to measure
the off-shell coupling strength of the Higgs boson. This
paper presents constraints on the off-shell Higgs boson
event yields normalised to the Standard Model prediction
(signal strength) in the [Formula: see text], [Formula: see
text] and [Formula: see text] final states. The result is
based on <i>pp</i> collision data collected by the ATLAS
experiment at the LHC, corresponding to an integrated
luminosity of 20.3 fb[Formula: see text] at a collision
energy of [Formula: see text] TeV. Using the [Formula: see
text] method, the observed 95 [Formula: see text]
confidence level (CL) upper limit on the off-shell signal
strength is in the range 5.1-8.6, with an expected range of
6.7-11.0. In each case the range is determined by varying
the unknown [Formula: see text] and [Formula: see text]
background K-factor from higher-order quantum chromodynamics
corrections between half and twice the value of the known
signal K-factor. Assuming the relevant Higgs boson couplings
are independent of the energy scale of the Higgs boson
production, a combination with the on-shell measurements
yields an observed (expected) 95 [Formula: see text] CL
upper limit on [Formula: see text] in the range 4.5-7.5
(6.5-11.2) using the same variations of the background
K-factor. Assuming that the unknown [Formula: see text]
background K-factor is equal to the signal K-factor, this
translates into an observed (expected) 95 [Formula: see
text] CL upper limit on the Higgs boson total width of 22.7
(33.0) MeV.},
Doi = {10.1140/epjc/s10052-015-3542-2},
Key = {fds321300}
}
@article{fds329809,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Armitage, LJ},
Title = {Correction to: Identification and rejection of pile-up jets
at high pseudorapidity with the ATLAS detector (Eur. Phys.
J. C, (2017), 77, (580), 10.1140/epjc/s10052-017-5081-5)},
Journal = {European Physical Journal C},
Volume = {77},
Number = {10},
Publisher = {Springer Nature America, Inc},
Year = {2017},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5245-3},
Abstract = {Unfortunately, in the original version of this article the
copyright holder was wrong in the HTML. The original article
has been corrected.},
Doi = {10.1140/epjc/s10052-017-5245-3},
Key = {fds329809}
}
@article{fds375953,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei,
D and Dos Santos and SPA and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Correlations between flow and transverse momentum in Xe + Xe
and Pb + Pb collisions at the LHC with the ATLAS detector: A
probe of the heavy-ion initial state and nuclear
deformation},
Journal = {Physical Review C},
Volume = {107},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevC.107.054910},
Abstract = {The correlations between flow harmonics vn for n = 2, 3, and
4 and mean transverse momentum [pT] in 129Xe + 129Xe and
208Pb + 208Pb collisions at √s = 5.44 and 5.02 TeV,
respectively, are measured using charged particles with the
ATLAS detector. The correlations are potentially sensitive
to the shape and size of the initial geometry, nuclear
deformation, and initial momentum anisotropy. The effects
from nonflow and centrality fluctuations are minimized,
respectively, via a subevent cumulant method and an
event-activity selection based on particle production at
very forward rapidity. The vn-[pT] correlations show strong
dependencies on centrality, harmonic number n, pT, and
pseudorapidity range. Current models qualitatively describe
the overall centrality- and system-dependent trends but fail
to quantitatively reproduce all features of the data. In
central collisions, where models generally show good
agreement, the v2-[pT] correlations are sensitive to the
triaxiality of the quadruple deformation. Comparison of the
model with the Pb + Pb and Xe + Xe data confirms that the
129Xe nucleus is a highly deformed triaxial ellipsoid that
has neither a prolate nor oblate shape. This provides strong
evidence for a triaxial deformation of the 129Xe nucleus
from high-energy heavy-ion collisions.},
Doi = {10.1103/PhysRevC.107.054910},
Key = {fds375953}
}
@article{fds331638,
Author = {al, TAE},
Title = {Cross section and heavy quark composition of gamma+ mu
events produced in pp collisions},
Journal = {Physical Review},
Volume = {D65},
Number = {1},
Pages = {012003},
Publisher = {American Physical Society (APS)},
Year = {2002},
url = {http://dx.doi.org/10.1103/PhysRevD.65.012003},
Abstract = {We present a measurement of the cross section and the first
measurement of the heavy flavor content of associated direct
photon 1 muon events produced in hadronic collisions. These
measurements come from a sample of 1.8 TeV pp̅ collisions
recorded with the Collider Detector at Fermilab. Quantum
chromodynamics (QCD) predicts that these events are
primarily due to the Compton scattering process cg→ γ+μ,
with the final-state charm quark producing a muon. The cross
section for events with a photon transverse momentum between
12 and 40 GeV/c is measured to be 46.8±6.3±7.5 pb, which
is two standard deviations below the most recent theoretical
calculation. A significant fraction of the events in the
sample contain a final-state bottom quark. The ratio of
charm to bottom production is measured to be 2.4±1.2, in
good agreement with QCD models.},
Doi = {10.1103/PhysRevD.65.012003},
Key = {fds331638}
}
@article{fds321170,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Dark matter interpretations of ATLAS searches for the
electroweak production of supersymmetric particles in √s=8
TeV proton-proton collisions},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {9},
Publisher = {Springer Nature},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2016)175},
Abstract = {A selection of searches by the ATLAS experiment at the LHC
for the electroweak production of SUSY particles are used to
study their impact on the constraints on dark matter
candidates. The searches use 20 fb−1 of proton-proton
collision data at s=8 TeV. A likelihood-driven scan of a
five-dimensional effective model focusing on the
gaugino-higgsino and Higgs sector of the phenomenological
minimal supersymmetric Standard Model is performed. This
scan uses data from direct dark matter detection
experiments, the relic dark matter density and precision
flavour physics results. Further constraints from the ATLAS
Higgs mass measurement and SUSY searches at LEP are also
applied. A subset of models selected from this scan are used
to assess the impact of the selected ATLAS searches in this
five-dimensional parameter space. These ATLAS searches
substantially impact those models for which the mass
m(χ˜10) of the lightest neutralino is less than 65 GeV,
excluding 86% of such models. The searches have limited
impact on models with larger m(χ˜10) due to either heavy
electroweakinos or compressed mass spectra where the mass
splittings between the produced particles and the lightest
supersymmetric particle is small.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP09(2016)175},
Key = {fds321170}
}
@article{fds321292,
Author = {ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Piqueras, DÁ and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Determination of spin and parity of the Higgs boson in the
[Formula: see text] decay channel with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {5},
Pages = {231},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3436-3},
Abstract = {Studies of the spin and parity quantum numbers of the Higgs
boson in the [Formula: see text] final state are presented,
based on proton-proton collision data collected by the ATLAS
detector at the Large Hadron Collider, corresponding to an
integrated luminosity of 20.3 fb[Formula: see text] at a
centre-of-mass energy of [Formula: see text] TeV. The
Standard Model spin-parity [Formula: see text] hypothesis is
compared with alternative hypotheses for both spin and CP.
The case where the observed resonance is a mixture of the
Standard-Model-like Higgs boson and CP-even ([Formula: see
text]) or CP-odd ([Formula: see text]) Higgs boson in
scenarios beyond the Standard Model is also studied. The
data are found to be consistent with the Standard Model
prediction and limits are placed on alternative spin and CP
hypotheses, including CP mixing in different
scenarios.},
Doi = {10.1140/epjc/s10052-015-3436-3},
Key = {fds321292}
}
@article{fds365390,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arguin, JF and Argyropoulos,
S},
Title = {Determination of the parton distribution functions of the
proton from ATLAS measurements of differential
W± and Z boson production in association with
jets},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2021)223},
Abstract = {This article presents a new set of proton parton
distribution functions, ATLASepWZVjet20, produced in an
analysis at next-to-next-to-leading order in QCD. The new
data sets considered are the measurements of W+ and W−
boson and Z boson production in association with jets in pp
collisions at s = 8 TeV performed by the ATLAS experiment at
the LHC with integrated luminosities of 20.2 fb−1 and 19.9
fb−1, respectively. The analysis also considers the ATLAS
measurements of differential W± and Z boson production at s
= 7 TeV with an integrated luminosity of 4.6 fb−1 and
deep-inelastic-scattering data from e±p collisions at the
HERA accelerator. An improved determination of the sea-quark
densities at high Bjorken x is shown, while confirming a
strange-quark density similar in size to the up- and
down-sea-quark densities in the range x ≲ 0.02 found by
previous ATLAS analyses. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP07(2021)223},
Key = {fds365390}
}
@article{fds365355,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
ATH},
Title = {Determination of the parton distribution functions of the
proton using diverse ATLAS data from pp collisions at √s=7
, 8 and 13 TeV},
Journal = {European Physical Journal C},
Volume = {82},
Number = {5},
Year = {2022},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10217-z},
Abstract = {This paper presents an analysis at next-to-next-to-leading
order in the theory of quantum chromodynamics for the
determination of a new set of proton parton distribution
functions using diverse measurements in pp collisions at
s=7, 8 and 13 TeV, performed by the ATLAS experiment at the
Large Hadron Collider, together with deep inelastic
scattering data from ep collisions at the HERA collider. The
ATLAS data sets considered are differential cross-section
measurements of inclusive W± and Z/ γ∗ boson production,
W± and Z boson production in association with jets, tt¯
production, inclusive jet production and direct photon
production. In the analysis, particular attention is paid to
the correlation of systematic uncertainties within and
between the various ATLAS data sets and to the impact of
model, theoretical and parameterisation uncertainties. The
resulting set of parton distribution functions is called
ATLASpdf21.},
Doi = {10.1140/epjc/s10052-022-10217-z},
Key = {fds365355}
}
@article{fds321212,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T},
Title = {Determination of the Ratio of b-Quark Fragmentation
Fractions f(s)/f(d) in pp Collisions at √s=7 TeV with
the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {115},
Number = {26},
Pages = {262001},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.115.262001},
Abstract = {With an integrated luminosity of 2.47 fb(-1) recorded
by the ATLAS experiment at the LHC, the exclusive decays
B(s)(0)→J/ψϕ and B(d)(0)→J/ψK(*0) of B mesons
produced in pp collisions at √s=7 TeV are used to
determine the ratio of fragmentation fractions f(s)/f(d).
From the observed B(s)(0)→J/ψϕ and B(d)(0)→J/ψK(*0)
yields, the quantity (f(s)/f(d))[B(B(s)(0)→J/ψϕ)/B(B(d)(0)→J/ψK(*0))]
is measured to be 0.199±0.004(stat)±0.008(syst). Using a
recent theory prediction for [B(B(s)(0)→J/ψϕ)/B(B(d)(0)→J/ψK(*0))]
yields (f(s)/f(d))=0.240±0.004(stat)±0.010(syst)±0.017(th).
This result is based on a new approach that provides a
significant improvement of the world average.},
Doi = {10.1103/physrevlett.115.262001},
Key = {fds321212}
}
@article{fds321220,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Determination of the top-quark pole mass using tt¯tt¯ +
1-jet events collected with the ATLAS experiment in 7 TeV pp
collisions},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {10},
Publisher = {Springer Nature},
Year = {2015},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2015)121},
Abstract = {Abstract: The normalized differential cross section for
top-quark pair production in association with at least one
jet is studied as a function of the inverse of the invariant
mass of the tt¯(Formula presented.) + 1-jet system. This
distribution can be used for a precise determination of the
top-quark mass since gluon radiation depends on the mass of
the quarks. The experimental analysis is based on
proton-proton collision data collected by the ATLAS detector
at the LHC with a centre-of-mass energy of 7 TeV
corresponding to an integrated luminosity of 4.6 fb−1. The
selected events were identified using the lepton+jets
top-quark-pair decay channel, where lepton refers to either
an electron or a muon. The observed distribution is compared
to a theoretical prediction at next-to-leading-order
accuracy in quantum chromodynamics using the pole-mass
scheme. With this method, the measured value of the
top-quark pole mass, mtpole, is:mtpole=173.7±1.5stat.±1.4syst.−0.5+1.0theoryGeV.(Formula
presented.). This result represents the most precise
measurement of the top-quark pole mass to date.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP10(2015)121},
Key = {fds321220}
}
@article{fds365413,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MM and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Differential cross-section measurements for the electroweak
production of dijets in association with a Z boson in
proton–proton collisions at ATLAS},
Journal = {European Physical Journal C},
Volume = {81},
Number = {2},
Year = {2021},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08734-w},
Abstract = {Differential cross-section measurements are presented for
the electroweak production of two jets in association with a
Z boson. These measurements are sensitive to the
vector-boson fusion production mechanism and provide a
fundamental test of the gauge structure of the Standard
Model. The analysis is performed using proton–proton
collision data collected by ATLAS at s=13TeV and with an
integrated luminosity of 139fb-1. The differential
cross-sections are measured in the Z→ ℓ+ℓ- decay
channel (ℓ= e, μ) as a function of four observables: the
dijet invariant mass, the rapidity interval spanned by the
two jets, the signed azimuthal angle between the two jets,
and the transverse momentum of the dilepton pair. The data
are corrected for the effects of detector inefficiency and
resolution and are sufficiently precise to distinguish
between different state-of-the-art theoretical predictions
calculated using Powheg+Pythia8, Herwig7+Vbfnlo and
Sherpa 2.2. The differential cross-sections are used to
search for anomalous weak-boson self-interactions using a
dimension-six effective field theory. The measurement of the
signed azimuthal angle between the two jets is found to be
particularly sensitive to the interference between the
Standard Model and dimension-six scattering amplitudes and
provides a direct test of charge-conjugation and parity
invariance in the weak-boson self-interactions.},
Doi = {10.1140/epjc/s10052-020-08734-w},
Key = {fds365413}
}
@article{fds321248,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
M},
Title = {Differential top-antitop cross-section measurements as a
function of observables constructed from final-state
particles using pp collisions at √s = 7 TeV in the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {6},
Pages = {1-56},
Publisher = {Springer Nature},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2015)100},
Abstract = {Abstract: Various differential cross-sections are measured
in top-quark pair (tt) events produced in proton-proton
collisions at a centre-of-mass energy of √s = 7 TeV at the
LHC with the ATLAS detector. These differential
cross-sections are presented in a data set corresponding to
an integrated luminosity of 4.6 fb−1. The differential
cross-sections are presented in terms of kinematic
variables, such as momentum, rapidity and invariant mass, of
a top-quark proxy referred to as the pseudo-top-quark as
well as the pseudo-top-quark pair system. The dependence of
the measurement on theoretical models is minimal. The
measurements are performed on tt events in the lepton+jets
channel, requiring exactly one charged lepton and at least
four jets with at least two of them tagged as originating
from a b-quark. The hadronic and leptonic pseudo-top-quarks
are defined via the leptonic or hadronic decay mode of the W
boson produced by the top-quark decay in events with a
single charged lepton. Differential cross-section
measurements of the pseudo-top-quark variables are compared
with several Monte Carlo models that implement
next-to-leading order or leading-order multi-leg
matrix-element calculations.},
Doi = {10.1007/JHEP06(2015)100},
Key = {fds321248}
}
@article{fds308505,
Author = {Aaltonen, and T, and others},
Title = {Diffractive $W$ and $Z$ production at the Fermilab
Tevatron},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {11},
Pages = {112004},
Publisher = {American Physical Society},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.82.112004},
Abstract = {We report on a measurement of the fraction of events with a
W or Z boson which are produced diffractively in p̄p
collisions at √s=1.96TeV, using data from 0.6fb⊃-1 of
integrated luminosity collected with the CDFII detector
equipped with a Roman-pot spectrometer that detects the p̄
from p̄+p→p̄+[X+W/Z]. We find that (1.00±0.11)% of Ws
and (0.88±0.22)% of Zs are produced diffractively in a
region of antiproton or proton fractional momentum loss ξ
of 0.03<ξ<0.10 and 4-momentum transferred squared t of
-1<t<0(GeV/c)2, where we account for the events in which the
proton scatters diffractively while the antiproton
dissociates, p̄+p→[X+W/Z]+p, by doubling the measured
proton dissociation fraction. We also report on searches for
W and Z production in double Pomeron exchange,
p+p̄→p+[X+W/Z]+p̄, and on exclusive Z production,
p̄+p→p̄+Z+p. No signal is seen above background for
these processes, and comparisons are made with expectations.
© 2010 The American Physical Society.},
Doi = {10.1103/PhysRevD.82.112004},
Key = {fds308505}
}
@article{fds308762,
Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Amaral, P and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Borras, K and Bortoletto, D and Boudreau,
J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, JY and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly, A and Convery, ME and Conway, J and Cordelli,
M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Dominguez, A and Donati, S and Done, J and D'Onofrio,
M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Erbacher, R and Errede, D and Errede, S and Fan, Q and Fang, HC and Feild,
RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman,
J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Glagolev, V and Glenzinski, D and Gold,
M and Goldstein, J and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher,
F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hollebeek, R and Holloway, L and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Ivanov, A and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
T and Karr, K and Kartal, S and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim,
YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Lee, AM and Lee, K and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, NS and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti, P and McFarland,
KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Miyazaki, Y and Moggi, N and Moore, C and Moore, E and Moore, R and Morita,
Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar,
A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Renton, P and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi,
L and Sato, H and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott,
A and Scribano, A and Sedov, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti, A and Siegrist,
J and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Steele,
J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, RJ and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thomson, E and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback,
D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Tsybychev, D and Turini,
N and Ukegawa, F and Vaiciulis, T and Valls, J and Vejcik, S and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Wang, SM and Ward, B and Waschke, S and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkes, T and Williams,
HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Diffractive dijet production at √s = 630 and 1800 GeV at
the Fermilab Tevatron},
Journal = {Physical Review Letters},
Volume = {88},
Number = {15},
Pages = {1518021-1518026},
Year = {2002},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.88.151802},
Abstract = {The diffractive dijet production at √s = 630 and 1800 GeV
at the Fermilab Tevatron was presented. The β and ξ
dependence of the diffractive structure function at √s =
1800 GeV and it was found that it obeyed β-ξ factorization
for β<0.5. Results showed that the ξ-0.9±0.1
dependence indicated that Pomeron-like behavior extended to
moderately high ξ values in diffractive dijet
production.},
Doi = {10.1103/physrevlett.88.151802},
Key = {fds308762}
}
@article{fds308397,
Author = {Aaltonen, T and Albrow, M and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F},
Title = {Diffractive dijet production in p̄p collisions at
√s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.86.032009},
Abstract = {We report on a study of diffractive dijet production in p̄p
collisions at √s=1.96TeV using the CDF II detector at the
Fermilab Tevatron p̄p collider. A data sample from 310pb -1
of integrated luminosity collected by triggering on a high
transverse energy jet, ETjet, in coincidence with a recoil
antiproton detected in a Roman pot spectrometer is used to
measure the ratio of single-diffractive to inclusive-dijet
event rates as a function of xp ̄ of the interacting parton
in the antiproton, the Bjorken-x, xBjp̄, and a Q2(ETjet)2
in the ranges 10 -3<xBjp̄<10 -1 and 102<Q2<104GeV2,
respectively. Results are presented for the region of
p̄-momentum-loss fraction 0.03<ξ p̄<0.09 and a
four-momentum transfer squared t p̄>-4GeV2. The t p̄
dependence is measured as a function of Q2 and xBjp̄ and
compared with that of inclusive single diffraction
dissociation. We find weak xBjp̄ and Q2 dependencies in the
ratio of single diffractive to inclusive event rates, and no
significant Q2 dependence in the diffractive t p̄
distributions. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.032009},
Key = {fds308397}
}
@article{fds308845,
Author = {al, FAE},
Title = {Dijet Production by Color-Singlet Exchange at the Fermilab
Tevatron},
Journal = {Phys. Rev. Lett.},
Volume = {80},
Number = {6},
Pages = {1156},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.1156},
Abstract = {We report a new measurement of dijet production by
color-singlet exchange in pp® collisions at √s = 1.8 TeV
at the Fermilab Tevatron. In a sample of events with two
jets of transverse energy EjetT > 20 GeV, pseudorapidity in
the range 1.8 < |ηjet| < 3.5, and η1η2 < 0, we find that
a fraction R = [1.13 ± 0.12(stat) ± 0.11(syst)]% has a
pseudorapidity gap within |η| < 1 between the jets that can
be attributed to color-singlet exchnage. The fraction R
shows no significant dependence on EjetT or on the
pseudorapidity separation between the jets. © 1998 American
Physical Society.},
Doi = {10.1103/PhysRevLett.80.1156},
Key = {fds308845}
}
@article{fds308534,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar, P and Beecher, D and Behari, S and Bellettini,
G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Copic, K and Cordelli, M and Cortiana, G and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni,
GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest,
R and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper,
S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Koay, SA and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao,
T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Movilla Fernandez and P and Mülmenstädt,
J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura,
K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert,
B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi,
F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers,
E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber,
I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer,
B},
Title = {Direct bound on the total decay width of the top quark in pp
collisions at sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {102},
Number = {4},
Pages = {042001},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.102.042001},
Abstract = {We present the first direct experimental bound on the total
decay width of the top quark, Gamma(t), using 955 pb(-1) of
the Tevatron's pp collisions recorded by the Collider
Detector at Fermilab. We identify 253 top-antitop pair
candidate events. The distribution of reconstructed top
quark mass from these events is fitted to templates
representing different values of the top quark width. Using
a confidence interval based on likelihood-ratio ordering, we
extract an upper limit at 95% C.L. of Gamma(t)<13.1 GeV for
an assumed top quark mass of 175 GeV/c(2).},
Doi = {10.1103/physrevlett.102.042001},
Key = {fds308534}
}
@article{fds365672,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei,
D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH},
Title = {Direct constraint on the Higgs–charm coupling from a
search for Higgs boson decays into charm quarks with the
ATLAS detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {8},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10588-3},
Abstract = {A search for the Higgs boson decaying into a pair of charm
quarks is presented. The analysis uses proton–proton
collisions to target the production of a Higgs boson in
association with a leptonically decaying W or Z boson. The
dataset delivered by the LHC at a centre-of-mass energy of
[InlineEquation not available: see fulltext.] and recorded
by the ATLAS detector corresponds to an integrated
luminosity of 139 fb-1. Flavour-tagging algorithms are used
to identify jets originating from the hadronisation of charm
quarks. The analysis method is validated with the
simultaneous measurement of WW, WZ and ZZ production, with
observed (expected) significances of 2.6 (2.2) standard
deviations above the background-only prediction for the (W/
Z) Z(→ cc¯) process and 3.8 (4.6) standard deviations for
the (W/ Z) W(→ cq) process. The (W/ Z) H(→ cc¯) search
yields an observed (expected) upper limit of 26 (31) times
the predicted Standard Model cross-section times branching
fraction for a Higgs boson with a mass of [InlineEquation
not available: see fulltext.], corresponding to an observed
(expected) constraint on the charm Yukawa coupling modifier
|κc|<8.5(12.4), at the 95% confidence level. A combination
with the ATLAS (W/ Z) H, H→ bb¯ analysis is performed,
allowing the ratio κc/ κb to be constrained to less than
4.5 at the 95% confidence level, smaller than the ratio of
the b- and c-quark masses, and therefore determines the
Higgs-charm coupling to be weaker than the Higgs-bottom
coupling at the 95% confidence level.},
Doi = {10.1140/epjc/s10052-022-10588-3},
Key = {fds365672}
}
@article{fds308301,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Direct measurement of the total decay width of the top
quark.},
Journal = {Physical review letters},
Volume = {111},
Number = {20},
Pages = {202001},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.111.202001},
Abstract = {We present a measurement of the total decay width of the top
quark using events with top-antitop quark pair candidates
reconstructed in the final state with one charged lepton and
four or more hadronic jets. We use the full Tevatron run II
data set of sqrt[s]=1.96 TeV proton-antiproton
collisions recorded by the CDF II detector. The top quark
mass and the mass of the hadronically decaying W boson are
reconstructed for each event and compared with distributions
derived from simulated signal and background samples to
extract the top quark width (Γtop) and the energy scale of
the calorimeter jets with in situ calibration. For a top
quark mass Mtop=172.5 GeV/c2, we find
1.10<Γtop<4.05 GeV at 68% confidence level, which is
in agreement with the standard model expectation of 1.3 GeV
and is the most precise direct measurement of the top quark
width to date.},
Doi = {10.1103/physrevlett.111.202001},
Key = {fds308301}
}
@article{fds340918,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and De
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Van Den
Brink and S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer,
E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and Dejongh, F and Dell'Agnello, S and Dell'Orso, M and Demina,
R},
Title = {Direct measurement of the W Boson width in pp̄ collisions
at √s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {85},
Number = {16},
Pages = {3347-3352},
Year = {2000},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevLett.85.3347},
Abstract = {The W boson width, ΓW obtained in studies of the
transverse-mass spectra of leptonic W decays is measured.
Through analysis, the W width is determined from a binned
log-likelihood fit to the transverse-mass distribution in
the region 100 < MT < 200 GeV. Including previously
published computational fluid dynamics (CDF) electron result
with the same common error yields ΓW = 2.05 ± 0.10(stat)
± 0.08(syst) GeV.},
Doi = {10.1103/PhysRevLett.85.3347},
Key = {fds340918}
}
@article{fds308905,
Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman,
J},
Title = {Direct measurement of the W boson width.},
Journal = {Physical review letters},
Volume = {74},
Number = {3},
Pages = {341-345},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.74.341},
Abstract = {This Letter describes a direct measurement of the W boson
decay width, Γ(W), using the high-mass tail of the
transverse mass spectrum of W→eν decays recorded by the
Collider Detector at Fermilab. We findΓ(W)=2.11±0.28(stat)±0.16(syst)
GeV and compare this direct measurement with indirect means
of obtaining the width. © 1995 The American Physical
Society.},
Doi = {10.1103/physrevlett.74.341},
Key = {fds308905}
}
@article{fds308527,
Author = {Aaltonen, T and others},
Title = {Direct Measurement of the W Production Charge Asymmetry in
pp̅ Collisions at sqrt[s] =1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {18},
Pages = {181801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.181801},
Abstract = {We present the first direct measurement of the W production
charge asymmetry as a function of the W boson rapidity yW in
pp̅ collisions at sqrt[s]=1.96 TeV. We use a sample of
W→eν events in data from 1 fb-1 of integrated
luminosity collected using the CDF II detector. In the
region |yW|<3.0, this measurement is capable of
constraining the ratio of up- and down-quark momentum
distributions in the proton more directly than in previous
measurements of the asymmetry that are functions of the
charged-lepton pseudorapidity.},
Doi = {10.1103/physrevlett.102.181801},
Key = {fds308527}
}
@article{fds308737,
Author = {al, DAE},
Title = {Direct photon cross section with conversions at
CDF},
Journal = {Physical Review},
Volume = {D70},
Number = {7},
Pages = {074008},
Publisher = {American Physical Society (APS)},
Year = {2004},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.70.074008},
Abstract = {0.9 using data collected between 1994 and 1995 by the
Collider Detector at Fermilab (CDF). The measurement is
based on events where the photon converts into an
electron-positron pair in the material of the inner
detector, resulting in a two track event signature. To
remove pi 0--> gamma gamma and eta --> gamma gamma events
from the data we use a new background subtraction technique
which takes advantage of the tracking information available
in a photon conversion event. We find that the shape of the
cross section as a function of photon pT is poorly described
by next-to- leading-order QCD predictions, but agrees with
previous CDF measurements.},
Doi = {10.1103/PhysRevD.70.074008},
Key = {fds308737}
}
@article{fds308663,
Author = {Abulencia, and A, and others},
Title = {Direct search for Dirac magnetic monopoles in $p\bar{p}$
collisions at $\sqrt{s} = 1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {20},
Pages = {201801},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.201801},
Abstract = {We search for pair-produced Dirac magnetic monopoles in 35.7
pb-1 of proton-antiproton collisions at s**(1/2) = 1.96 TeV
with the Collider Detector at Fermilab (CDF). We find no
monopole candidates corresponding to a 95\% confidence-level
cross-section limit sigma 360 GeV/c2.},
Doi = {10.1103/physrevlett.96.201801},
Key = {fds308663}
}
@article{fds308469,
Author = {Aaltonen, and T, and others},
Title = {Direct Top-Quark Width Measurement at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {23},
Pages = {232003},
Publisher = {American Physical Society},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.232003},
Abstract = {We present a measurement of the top-quark width in the
lepton+jets decay channel of tt events produced in p p
collisions at Fermilab's Tevatron collider and collected by
the CDF II detector. From a data sample corresponding to 4.3
fb(-1) of integrated luminosity, we identify 756 candidate
events. The top-quark mass and the mass of the hadronically
decaying W boson that comes from the top-quark decay are
reconstructed for each event and compared with templates of
different top-quark widths (Γ(t)) and deviations from
nominal jet energy scale (Δ(JES)) to perform a simultaneous
fit for both parameters, where Δ(JES) is used for the in
situ calibration of the jet energy scale. By applying a
Feldman-Cousins approach, we establish an upper limit at 95%
confidence level (CL) of Γ(t) <7.6 GeV and a two-sided 68%
CL interval of 0.3 GeV <Γ(t) <4.4 GeV for a top-quark
mass of 172.5 GeV/c(2), which are consistent with the
standard model prediction.},
Doi = {10.1103/PhysRevLett.105.232003},
Key = {fds308469}
}
@article{fds308861,
Author = {al, FAE},
Title = {Double parton scattering in (p)over-bar-p collisions at root
s=1.8 TeV},
Journal = {Phys. Rev. D},
Volume = {56},
Number = {7},
Pages = {3811-3832},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.56.3811},
Abstract = {A strong signal for double parton (DP) scattering is
observed in a [Formula presented] sample of [Formula
presented] data from the CDF experiment at the Fermilab
Tevatron. In DP events, two separate hard scatterings take
place in a single [Formula presented] collision. We isolate
a large sample of data [Formula presented] of which 53% are
found to be DP. The process-independent parameter of double
parton scattering, [Formula presented] is obtained without
reference to theoretical calculations by comparing observed
DP events to events with hard scatterings in separate
[Formula presented] collisions. The result [Formula
presented] represents a significant improvement over
previous measurements, and is used to constrain simple
models of parton spatial density. The Feynman [Formula
presented] dependence of [Formula presented] is investigated
and none is apparent. Further, no evidence is found for
kinematic correlations between the two scatterings in DP
events. © 1997 The American Physical Society.},
Doi = {10.1103/PhysRevD.56.3811},
Key = {fds308861}
}
@article{fds308361,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach,
AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes,
JB and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey,
DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, JB and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Armadans,
RC and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung,
SL and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow,
BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu,
ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca,
D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron,
ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
RN and Clemens, JC},
Title = {Dynamics of isolated-photon plus jet production in pp
collisions at s=7 TeV with the ATLAS detector},
Journal = {Nuclear Physics B},
Volume = {875},
Number = {3},
Pages = {483-535},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.nuclphysb.2013.07.025},
Abstract = {The dynamics of isolated-photon plus jet production in pp
collisions at a centre-of-mass energy of 7 TeV has been
studied with the ATLAS detector at the LHC using an
integrated luminosity of 37 pb-1. Measurements of
isolated-photon plus jet bin-averaged cross sections are
presented as functions of photon transverse energy, jet
transverse momentum and jet rapidity. In addition, the
bin-averaged cross sections as functions of the difference
between the azimuthal angles of the photon and the jet, the
photon-jet invariant mass and the scattering angle in the
photon-jet centre-of-mass frame have been measured.
Next-to-leading-order QCD calculations are compared to the
measurements and provide a good description of the data,
except for the case of the azimuthal opening angle. © 2013
CERN.},
Doi = {10.1016/j.nuclphysb.2013.07.025},
Key = {fds308361}
}
@article{fds321328,
Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Electron and photon energy calibration with the ATLAS
detector using LHC Run 1 data},
Journal = {European Physical Journal C},
Volume = {74},
Number = {10},
Pages = {1-48},
Publisher = {Springer Nature},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3071-4},
Abstract = {This paper presents the electron and photon energy
calibration achieved with the ATLAS detector using about
25 fb-1 of LHC proton–proton collision data taken at
centre-of-mass energies of (Equation Present) and 8 TeV.
The reconstruction of electron and photon energies is
optimised using multivariate algorithms. The response of the
calorimeter layers is equalised in data and simulation, and
the longitudinal profile of the electromagnetic showers is
exploited to estimate the passive material in front of the
calorimeter and reoptimise the detector simulation. After
all corrections, the Z resonance is used to set the absolute
energy scale. For electrons from Z decays, the achieved
calibration is typically accurate to 0.05 % in most of the
detector acceptance, rising to 0.2 % in regions with large
amounts of passive material. The remaining inaccuracy is
less than 0.2–1 % for electrons with a transverse energy
of 10 GeV, and is on average 0.3 % for photons. The
detector resolution is determined with a relative inaccuracy
of less than 10 % for electrons and photons up to 60 GeV
transverse energy, rising to 40 % for transverse energies
above 500 GeV.},
Doi = {10.1140/epjc/s10052-014-3071-4},
Key = {fds321328}
}
@article{fds321358,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov,
AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau,
M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji,
W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and De Mendizabal,
JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet,
NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov,
G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Renstrom, PABD and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Cameron, D and Caminada, LM and Armadans, RC and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cantero, J and Cantrill,
R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland,
W},
Title = {Electron reconstruction and identification efficiency
measurements with the ATLAS detector using the 2011 LHC
proton-proton collision data.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {7},
Pages = {2941},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-2941-0},
Abstract = {Many of the interesting physics processes to be measured at
the LHC have a signature involving one or more isolated
electrons. The electron reconstruction and identification
efficiencies of the ATLAS detector at the LHC have been
evaluated using proton-proton collision data collected in
2011 at [Formula: see text] TeV and corresponding to an
integrated luminosity of 4.7 fb[Formula: see text].
Tag-and-probe methods using events with leptonic decays of
[Formula: see text] and [Formula: see text] bosons and
[Formula: see text] mesons are employed to benchmark these
performance parameters. The combination of all measurements
results in identification efficiencies determined with an
accuracy at the few per mil level for electron transverse
energy greater than 30 GeV.},
Doi = {10.1140/epjc/s10052-014-2941-0},
Key = {fds321358}
}
@article{fds365350,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei,
D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arguin, JF},
Title = {Emulating the impact of additional proton–proton
interactions in the ATLAS simulation by presampling sets of
inelastic Monte Carlo events},
Journal = {Computing and Software for Big Science},
Volume = {6},
Number = {1},
Year = {2022},
Month = {December},
url = {http://dx.doi.org/10.1007/s41781-021-00062-2},
Abstract = {The accurate simulation of additional interactions at the
ATLAS experiment for the analysis of proton–proton
collisions delivered by the Large Hadron Collider presents a
significant challenge to the computing resources. During the
LHC Run 2 (2015–2018), there were up to 70 inelastic
interactions per bunch crossing, which need to be accounted
for in Monte Carlo (MC) production. In this document, a new
method to account for these additional interactions in the
simulation chain is described. Instead of sampling the
inelastic interactions and adding their energy deposits to a
hard-scatter interaction one-by-one, the inelastic
interactions are presampled, independent of the hard
scatter, and stored as combined events. Consequently, for
each hard-scatter interaction, only one such presampled
event needs to be added as part of the simulation chain. For
the Run 2 simulation chain, with an average of 35
interactions per bunch crossing, this new method provides a
substantial reduction in MC production CPU needs of around
20%, while reproducing the properties of the reconstructed
quantities relevant for physics analyses with good
accuracy.},
Doi = {10.1007/s41781-021-00062-2},
Key = {fds365350}
}
@article{fds314184,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Erratum : Measurement of the inclusive jet cross-section in
proton-proton collisions at √s = 7 TeV using 4.5
fb−1 of data with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {9},
Pages = {1-39},
Publisher = {Springer Nature},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2015)141},
Abstract = {Abstract: It was found that the non-perturbative corrections
calculated using Pythia with the Perugia 2011 tune did not
include the effect of the underlying event. The affected
correction factors were recomputed using the Pythia 6.427
generator. These corrections are applied as baseline to the
NLO pQCD calculations and thus the central values of the
theoretical predictions have changed by a few percent with
the new corrections. This has a minor impact on the
agreement between the data and the theoretical predictions.
Figures 2 and 6 to 13, and all the tables have been updated
with the new values. A few sentences in the discussion in
sections 5.2 and 9 were altered or removed.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP09(2015)141},
Key = {fds314184}
}
@article{fds314852,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Erratum to ATLAS Run 1 searches for direct pair production
of third-generation squarks at the Large Hadron
Collider},
Journal = {European Physical Journal C},
Volume = {76},
Number = {3},
Publisher = {Springer Nature},
Year = {2016},
Month = {March},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-3935-x},
Doi = {10.1140/epjc/s10052-016-3935-x},
Key = {fds314852}
}
@article{fds365418,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
C},
Title = {Erratum to: Higgs boson production cross-section
measurements and their EFT interpretation in the 4 ℓ decay
channel at s = 13 TeV with the ATLAS detector (The European
Physical Journal C, (2020), 80, 10, (957),
10.1140/epjc/s10052-020-8227-9)},
Journal = {European Physical Journal C},
Volume = {81},
Number = {1},
Year = {2021},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08644-x},
Abstract = {In the published HTML version of this article, the
affiliations of the authors of the National Research Nuclear
University MEPhI, Moscow, Russia were unfortunately marked
incorrectly.},
Doi = {10.1140/epjc/s10052-020-08644-x},
Key = {fds365418}
}
@article{fds365398,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
C},
Title = {Erratum to: Higgs boson production cross-section
measurements and their EFT interpretation in the 4 ℓ decay
channel at s = 13 TeV with the ATLAS detector (The European
Physical Journal C, (2020), 80, 10, (957),
10.1140/epjc/s10052-020-8227-9)},
Journal = {European Physical Journal C},
Volume = {81},
Number = {5},
Year = {2021},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09116-6},
Abstract = {When quoting the final cross section result in the text of
the paper (Eur. Phys. J. C 80 (2020) 957), the theory
component of the uncertainty was incorrectly set to 0.04 pb
while the correct value of 0.03 pb was given in Table 8 and
in all other results reported in this paper.},
Doi = {10.1140/epjc/s10052-021-09116-6},
Key = {fds365398}
}
@article{fds365369,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Erratum to: Measurement of hadronic event shapes in high-p
T multijet final states at s = 13 TeV with the
ATLAS detector (Journal of High Energy Physics, (2021),
2021, 1, (188), 10.1007/JHEP01(2021)188)},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {12},
Year = {2021},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2021)053},
Abstract = {An error in the normalization of the Aplanarity and
D-parameter has been found. Insufficient precision on the
eigenvalue calculation can cause λ3 to be negative,
exclusively in two-jet events, yielding an underestimation
of the inclusive two-jet cross section.},
Doi = {10.1007/JHEP12(2021)053},
Key = {fds365369}
}
@article{fds365372,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Erratum to: Measurement of light-by-light scattering and
search for axion-like particles with 2.2 nb −1
of Pb+Pb data with the ATLAS detector (Journal of High
Energy Physics, (2021), 2021, 3, (243), 10.1007/JHEP03(2021)243)},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2021)050},
Abstract = {One correction is noted for the paper, which does not affect
the results reported. The right panel of figure 9 is
corrected as it contained the “internal” label, giving
the misleading impression on the credibility of the
figure.},
Doi = {10.1007/JHEP11(2021)050},
Key = {fds365372}
}
@article{fds321227,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Erratum to: Search for new phenomena in final states with an
energetic jet and large missing transverse momentum in pp
collisions at √s=8 TeV with the ATLAS detector (Eur. Phys.
J. C (2015) 75:299, 10.1140/epjc/s10052-015-3517-3)},
Journal = {European Physical Journal C},
Volume = {75},
Number = {9},
Publisher = {Springer Nature},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3639-7},
Doi = {10.1140/epjc/s10052-015-3639-7},
Key = {fds321227}
}
@article{fds365409,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Erratum to: Search for phenomena beyond the Standard Model
in events with large b-jet multiplicity using the ATLAS
detector at the LHC (The European Physical Journal C,
(2021), 81, 1, (11), 10.1140/epjc/s10052-020-08730-0)},
Journal = {European Physical Journal C},
Volume = {81},
Number = {3},
Year = {2021},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-08970-8},
Abstract = {In the original HTML version of this article, one
affiliation of the author V. O. Tikhomirov was missing. He
is affiliated to the following two affiliations: P.N.
Lebedev Physical Institute of the Russian Academy of
Sciences, Moscow, Russia National Research Nuclear
University MEPhI, Moscow, Russia The original article has
been corrected.},
Doi = {10.1140/epjc/s10052-021-08970-8},
Key = {fds365409}
}
@article{fds365378,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Erratum to: Search for squarks and gluinos in final states
with one isolated lepton, jets, and missing transverse
momentum at √s = 13 TeV with the ATLAS detector (The
European Physical Journal C, (2021), 81, 7, (600),
10.1140/epjc/s10052-021-09344-w)},
Journal = {European Physical Journal C},
Volume = {81},
Number = {10},
Year = {2021},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09748-8},
Abstract = {In this article the title was incorrectly given as ‘Search
for squarks and gluinos in final states with one isolated
lepton, jets, and missing transverse momentum at √s = 13
with the ATLAS detector’ but should have been ‘Search
for squarks and gluinos in final states with one isolated
lepton, jets, and missing transverse momentum at √s = 13
TeV with the ATLAS detector’. The original article has
been corrected.},
Doi = {10.1140/epjc/s10052-021-09748-8},
Key = {fds365378}
}
@article{fds314186,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Erratum to: Search for supersymmetry in events containing a
same-flavour opposite-sign dilepton pair, jets, and large
missing transverse momentum in √s = 8 TeV pp collisions
with the ATLAS detector (Eur. Phys. J. C, (2015), 75, (318),
10.1140/epjc/s10052-015-3518-2)},
Journal = {European Physical Journal C},
Volume = {75},
Number = {10},
Publisher = {Springer Nature},
Year = {2015},
Month = {October},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3661-9},
Doi = {10.1140/epjc/s10052-015-3661-9},
Key = {fds314186}
}
@article{fds314853,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Erratum to: Study of the spin and parity of the Higgs boson
in diboson decays with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {76},
Number = {3},
Publisher = {Springer Nature},
Year = {2016},
Month = {March},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-3934-y},
Doi = {10.1140/epjc/s10052-016-3934-y},
Key = {fds314853}
}
@article{fds311481,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Erratum: Indirect measurement of sin-2θW
(MW) using e+e - pairs in
the Z-boson region with pp̄ collisions at a
center-of-momentum energy of 1.96 TeV (Physical Review D
(2013) 88 (072002))},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.88.079905},
Doi = {10.1103/PhysRevD.88.079905},
Key = {fds311481}
}
@article{fds308491,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D},
Title = {Erratum: Measurement of particle production and inclusive
differential cross sections in pp̄ collisions at
√s=1.96TeV (Physical Review D - Particles, Fields,
Gravitation and Cosmology)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {82},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.82.119903},
Doi = {10.1103/PhysRevD.82.119903},
Key = {fds308491}
}
@article{fds308540,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
Title = {Erratum: Measurement of the inclusive jet cross section at
the Fermilab Tevatron pp̄ collider using a cone-based jet
algorithm (Physical Review D (2008) 78 (052006))},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.79.119902},
Doi = {10.1103/PhysRevD.79.119902},
Key = {fds308540}
}
@article{fds308766,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman,
J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria,
S},
Title = {Erratum: Measurement of the inclusive jet cross section in
pp collisions at √s= 1.8 Tev (Physical Review D-
Particles, Fields, Gravitation and Cosmology (2001) 64
(032001)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {65},
Number = {3},
Pages = {399031},
Year = {2002},
Month = {February},
Key = {fds308766}
}
@article{fds308647,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
MA},
Title = {Erratum: Measurement of the inclusive jet cross section
using the kT algorithm in pp̄ collisions at s=1.96TeV with
the CDF II detector (Physical Review D - Particles, Fields,
Gravitation and Cosmology (2007) 75, (092006))},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {75},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2007},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.75.119901},
Doi = {10.1103/PhysRevD.75.119901},
Key = {fds308647}
}
@article{fds308754,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman,
J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria,
S},
Title = {Erratum: Measurement of the tt̄ production cross in pp̄
collisions at √s= 1.8 Tev (Physical Review D (2001) 64
(32002))},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {67},
Number = {11},
Pages = {1199011-1199012},
Year = {2003},
Month = {June},
Key = {fds308754}
}
@article{fds308767,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman,
J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria,
S},
Title = {Erratum: Measurement of the two-jet differential cross
section in pp collisions at √s=1800 GeV (Physical Review
D- Particles, Fields, Gravitation and Cosmology (2001) 64
(012001)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {65},
Number = {3},
Pages = {399021},
Year = {2002},
Month = {February},
Key = {fds308767}
}
@article{fds308724,
Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
J and Culbertson, R and Dagenhart, D and D'Auria, S and De Barbaro and P and De Cecco and S and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi,
C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede,
S},
Title = {Erratum: Measurement of the W boson polarization in top
decay at CDF at √s p = 1:8 TeV (Physical Review D (2005)
71 (031101))},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {5},
Pages = {1-2},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.71.059901},
Doi = {10.1103/PhysRevD.71.059901},
Key = {fds308724}
}
@article{fds308493,
Author = {Aaltonen, T and Adelman, J and Álvarez Gonzalez, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M},
Title = {Erratum: Measurement of the W+W-
production cross section and search for anomalous WWγ and
WWZ couplings in pp̄ collisions at √s=1.96 TeV (Phys.
Rev. Lett. (2010) 104 (201801))},
Journal = {Physical Review Letters},
Volume = {105},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2010},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.019905},
Doi = {10.1103/PhysRevLett.105.019905},
Key = {fds308493}
}
@article{fds308372,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and D'Errico, M},
Title = {Erratum: Novel inclusive search for the Higgs boson in the
four-lepton final state at CDF (Physical Review D (2012) 86
(072012) DOI:10.1103/PhysRevD. 86.072012)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {9},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.86.099902},
Doi = {10.1103/PhysRevD.86.099902},
Key = {fds308372}
}
@article{fds308908,
Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and De
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Cihangir, S and Clark,
AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli,
M and Crane, D and Cunningham, JD and Daniels, T and DeJongh, F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dickson, M and Donati, S and Drucker, RB and Dunn, A and Einsweiler, K and Elias, JE and Ely, R and Engels, E and Eno, S and Errede, D and Errede, S and Fan, Q and Farhat, B and Fiori, I},
Title = {Erratum: Precision measurement of the prompt photon cross
section in pp collisions at s=1.8 TeV (Physical Review
Letters(1995) 74, 10 (1891-1893))},
Journal = {Physical Review Letters},
Volume = {74},
Number = {10},
Pages = {1891-1893},
Year = {1995},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevLett.74.1891},
Doi = {10.1103/PhysRevLett.74.1891},
Key = {fds308908}
}
@article{fds308705,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH},
Title = {Erratum: Search for Bs0 → μ+μ and Bd0 → μ+μ decays
in pp_ collisions with CDF II (Phys. Rev. Lett. (2005) 95
(221805))},
Journal = {Physical Review Letters},
Volume = {95},
Number = {24},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevLett.95.249905},
Doi = {10.1103/PhysRevLett.95.249905},
Key = {fds308705}
}
@article{fds335599,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Erratum: Search for Bs0 →μ+μ- and B0 →μ+μ- decays
with the full CDF Run II data set (Physical Review D (2013)
87 (072003) DOI: 10.1103/PhysRevD.87.072003)},
Journal = {Physical Review D},
Volume = {97},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2018},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.97.099901},
Abstract = {V. Krutelyov, of Texas A&M University and the University of
California at Santa Barbara, was erroneously omitted from
the author list.},
Doi = {10.1103/PhysRevD.97.099901},
Key = {fds335599}
}
@article{fds329811,
Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Sperka, D and Squillacioti, P and Stancari, M and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang, YC},
Title = {Erratum: Search for Bs0→μ+μ- and
B0→μ+μ- decays with CDF II
(Physical Review Letters (2011) 107 (191801))},
Journal = {Physical Review Letters},
Volume = {107},
Number = {23},
Year = {2011},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.239903},
Doi = {10.1103/PhysRevLett.107.239903},
Key = {fds329811}
}
@article{fds308545,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell,
M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A},
Title = {Erratum: Search for high-mass e+e- Resonances in pp̄
collisions at s=1.96TeV (Physical Review Letters (2009) 102
(031801))},
Journal = {Physical Review Letters},
Volume = {102},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevLett.102.059901},
Doi = {10.1103/PhysRevLett.102.059901},
Key = {fds308545}
}
@article{fds365402,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
Title = {Erratum: Search for new non-resonant phenomena in high-mass
dilepton final states with the ATLAS detector (Journal of
High Energy Physics, (2020), 2020, 11, (5),
10.1007/JHEP11(2020)005)},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2021)142},
Abstract = {The Lagrangian in eq. (2.1) of JHEP11 (2020) 005 has an
erroneous factor of 1/2. The analysis code used for the
results reported in the paper does not have this factor. The
results remain unchanged.},
Doi = {10.1007/JHEP04(2021)142},
Key = {fds365402}
}
@article{fds308290,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Erratum: Search for new phenomena in final states with large
jet multiplicities and missing transverse momentum at √s =
8 TeV proton-proton collisions using the ATLAS experiment
(Journal of High Energy Physics (2013) 10
(130))},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {1},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2014)109},
Doi = {10.1007/JHEP01(2014)109},
Key = {fds308290}
}
@article{fds308599,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
Gonzalez, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
Title = {Erratum: Search for pair production of scalar top quarks
decaying to a τ Lepton and a b quark in pp̄ collisions at
s=1.96TeV (Physical Review Letters (2008) 101
(071802))},
Journal = {Physical Review Letters},
Volume = {101},
Number = {8},
Publisher = {American Physical Society (APS)},
Year = {2008},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevLett.101.089901},
Doi = {10.1103/PhysRevLett.101.089901},
Key = {fds308599}
}
@article{fds321236,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Ålkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Erratum: Search for production of WW/WZ resonances decaying
to a lepton, neutrino and jets in pp collisions at √s = 8
TeV with the ATLAS detector (The European Physical Journal C
(2015) 75 (209) DOI: 10.1140/epjc/s10052-015-3425-6)},
Journal = {European Physical Journal C},
Volume = {75},
Number = {8},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3593-4},
Doi = {10.1140/epjc/s10052-015-3593-4},
Key = {fds321236}
}
@article{fds308827,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
AG and Cobal, M and Cocca, E and Contreras, M and Convery, ME and Conway,
J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and Jongh, FD and dell'Agnello, S and dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, W and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch,
H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel,
O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo,
RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster,
M and Lanzoni, M and Latino, G and Compte, TL and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntrye, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Mesropian, C and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato,
H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore,
E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg,
D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith,
C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella,
F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka, M and Tannenbaum,
B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto,
Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk,
W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal,
R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson,
R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Events with a rapidity gap between jets in p̄p collisions
at √s = 630 GeV},
Journal = {Physical Review Letters},
Volume = {81},
Number = {24},
Pages = {5278-5283},
Year = {1998},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.5278},
Abstract = {We report a measurement of the fraction of dijet events with
a rapidity gap between jets produced by color-singlet
exchange in p̄p collisions at √S = 630 GeV at the
Fermilab Tevatron. In events with two jets of transverse
energy ETjet > 8 GeV, pseudorapidity in the range 1.8
< |ηjet| < 3.5 and η1η2 < 0, the color-singlet
exchange fraction is found to be R = [2.7 ± 0.7(stat) ±
0.6(syst)]%. Comparisons are made with results obtained at
√s = 1800 GeV and with theoretical expectations.},
Doi = {10.1103/PhysRevLett.81.5278},
Key = {fds308827}
}
@article{fds308308,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger,
J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz,
D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Evidence for a bottom baryon resonance Λb*0 in CDF
data},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {7},
Pages = {071101},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.88.071101},
Abstract = {Using data from proton-antiproton collisions at √s=1.96
TeV recorded by the CDF II detector at the Fermilab
Tevatron, evidence for the excited resonance state Λb*0 is
presented in its Λb0π -π+ decay followed by the Λb0→Λ
c+π- and Λc+→pK-π+ decays. The analysis is based on a
data sample corresponding to an integrated luminosity of 9.6
fb-1 collected by an online event selection based on
charged-particle tracks displaced from the proton-antiproton
interaction point. The significance of the observed signal
is 3.5σ. The mass of the observed state is found to be
5919.22±0.76 MeV/c2 in agreement with similar findings in
proton-proton collision experiments. © 2013 American
Physical Society.},
Doi = {10.1103/PhysRevD.88.071101},
Key = {fds308308}
}
@article{fds308454,
Author = {Aaltonen, and T, and al, E},
Title = {Evidence for a mass dependent forward-backward asymmetry in
top quark pair production},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {11},
Pages = {112003},
Publisher = {American Physical Society},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.83.112003},
Abstract = {We present a new measurement of the inclusive
forward-backward tt̄ production asymmetry and its rapidity
and mass dependence. The measurements are performed with
data corresponding to an integrated luminosity of 5.3fb -1
of pp̄ collisions at √s=1.96TeV, recorded with the CDF-II
Detector at the Fermilab Tevatron. Significant inclusive
asymmetries are observed in both the laboratory frame and
the tt̄ rest frame, and in both cases are found to be
consistent with CP conservation under interchange of t and
t̄. In the tt̄ rest frame, the asymmetry is observed to
increase with the tt̄ rapidity difference, Δy, and with
the invariant mass M tt̄ of the tt̄ system. Fully
corrected parton-level asymmetries are derived in two
regions of each variable, and the asymmetry is found to be
most significant at large Δy and Mtt̄. For
Mtt̄?450GeV/c2, the parton-level asymmetry in the tt̄ rest
frame is Att̄=0.475±0.114 compared to a next-to-leading
order QCD prediction of 0.088±0.013. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevD.83.112003},
Key = {fds308454}
}
@article{fds308566,
Author = {Aaltonen, T and others},
Title = {Evidence for a Narrow Near-Threshold Structure in the J/ψϕ
Mass Spectrum in B+→J/ψϕK+ Decays},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {24},
Pages = {242002},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.242002},
Abstract = {Evidence is reported for a narrow structure near the J/ψϕ
threshold in exclusive B+→J/ψϕK+ decays produced in p̅
p collisions at sqrt[s]=1.96 TeV. A signal of 14
± 5 events, with statistical significance in excess
of 3.8 standard deviations, is observed in a data sample
corresponding to an integrated luminosity of 2.7 fb-1,
collected by the CDF II detector. The mass and natural width
of the structure are measured to be 4143.0 ±
2.9(stat) ± 1.2(syst) MeV/c2 and
11.7-5.0+8.3(stat) ± 3.7(syst) MeV/c2.},
Doi = {10.1103/physrevlett.102.242002},
Key = {fds308566}
}
@article{fds308384,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler,
M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto,
G and Bussey, P and Buszello, CP and Buzatu, A and Calamba, A and Calancha,
C and Camacho-Pérez, E and Camarda, S and Campanelli, M and Campbell,
M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo,
S and Carron, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chakrabarti, S and Chakraborty, D and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chevalier-Théry,
S and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, DK and Cho,
K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Chung, WH and Chung, YS and Cihangir, S and Ciocci, MA and Claes, D and Clark, A and Clarke, C and Clutter, J and Compostella, G and Convery, ME and Conway,
J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox, CA and Cox, DJ and Crescioli, F and Croc, A and Cuevas, J and Culbertson, R and Cutts, D and Dagenhart, D and d'Ascenzo, N and Das, A and Datta, M and Davies, G and de Barbaro, P and de
Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Dell'orso, M and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
SP and d'Errico, M and Desai, S and Deterre, C and Devaughan, K and Devoto,
F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
PF and Dittmann, JR and Dominguez, A and Donati, S and Dong, P and D'Onofrio, M and Dorigo, M and Dorigo, T and Dubey, A and Dudko, LV and Duggan, D and Duperrin, A and Dutt, S and Dyshkant, A and Eads, M and Ebina, K and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Evans, H and Evdokimov, A and Evdokimov, VN and Facini, G and Farrington, S and Feindt, M and Feng, L and Ferbel, T and Fernandez, JP and Ferrazza, C and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Frank, MJ and Franklin, M and Freeman, JC and Fuess, S and Funakoshi, Y and Gallinaro, M and Garcia-Bellido, A and Garcia, JE and García-González, JA and García-Guerra, GA and Garfinkel, AF and Garosi, P and Gavrilov, V and Gay, P and Geng, W and Gerbaudo, D and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Golovanov, G and Gomez-Ceballos, G and Gomez, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Goussiou, A and Grannis, PD and Greder, S and Greenlee,
H and Grenier, G and Grinstein, S and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hagopian, S and Hahn, SR and Haley, J and Halkiadakis, E and Hamaguchi, A and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, D and Hare, M and Harel, A and Harr, RF and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Heck, M and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hewamanage, S and Hildreth,
MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen,
B and Hogan, J and Hohlfeld, M and Hopkins, W and Horn, D and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeans, DT and Jeon, EJ and Jeong,
MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere, A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung, AW and Junk, TR and Juste, A and Kaadze, K and Kajfasz, E and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kasper, PA and Kato, Y and Katsanos, I and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava,
A and Kharzheev, YN and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim,
YK and Kimura, N and Kirby, M and Kiselevich, I and Klimenko, S and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Krop,
D and Kruse, M and Krutelyov, V and Kuhr, T and Kulikov, S and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lammers, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lebrun, P and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li,
H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Lin,
C-J and Lindgren, M and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lubatti, HJ and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lysak, R and Lys, J and Maciel, AKA and Madar, R and Madrak,
R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G},
Title = {Evidence for a particle produced in association with weak
bosons and decaying to a bottom-antibottom quark pair in
higgs boson searches at the tevatron.},
Journal = {Physical review letters},
Volume = {109},
Number = {7},
Pages = {071804},
Year = {2012},
Month = {August},
url = {http://inspirehep.net/record/1124036},
Abstract = {We combine searches by the CDF and D0 Collaborations for the
associated production of a Higgs boson with a W or Z boson
and subsequent decay of the Higgs boson to a
bottom-antibottom quark pair. The data, originating from
Fermilab Tevatron pp collisions at √s = 1.96 TeV,
correspond to integrated luminosities of up to 9.7 fb(-1).
The searches are conducted for a Higgs boson with mass in
the range 100-150 GeV/c(2). We observe an excess of events
in the data compared with the background predictions, which
is most significant in the mass range between 120 and 135
GeV/c(2). The largest local significance is 3.3 standard
deviations, corresponding to a global significance of 3.1
standard deviations. We interpret this as evidence for the
presence of a new particle consistent with the standard
model Higgs boson, which is produced in association with a
weak vector boson and decays to a bottom-antibottom quark
pair.},
Doi = {10.1103/physrevlett.109.071804},
Key = {fds308384}
}
@article{fds321323,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baker,
S and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, MF and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch,
A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y},
Title = {Evidence for electroweak production of W±W±jj in pp
collisions at sqrt[s] = 8 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {113},
Number = {14},
Pages = {141803},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.113.141803},
Abstract = {This Letter presents the first study of W(±)W(±)jj,
same-electric-charge diboson production in association with
two jets, using 20.3 fb(-1) of proton-proton collision data
at sqrt[s] = 8 TeV recorded by the ATLAS detector at
the Large Hadron Collider. Events with two reconstructed
same-charge leptons (e(±)e(±), e(±)μ(±), and
μ(±)μ(±)) and two or more jets are analyzed. Production
cross sections are measured in two fiducial regions, with
different sensitivities to the electroweak and strong
production mechanisms. First evidence for W(±)W(±)jj
production and electroweak-only W(±)W(±)jj production is
observed with a significance of 4.5 and 3.6 standard
deviations, respectively. The measured production cross
sections are in agreement with standard model predictions.
Limits at 95% confidence level are set on anomalous quartic
gauge couplings.},
Doi = {10.1103/physrevlett.113.141803},
Key = {fds321323}
}
@article{fds308268,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Vázquez, F and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Evidence for s-channel single-top-quark production in events
with one charged lepton and two jets at CDF.},
Journal = {Physical review letters},
Volume = {112},
Number = {23},
Pages = {231804},
Year = {2014},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.112.231804},
Abstract = {We report evidence for s-channel single-top-quark production
in proton-antiproton collisions at center-of-mass energy
sqrt[s] = 1.96 TeV using a data set that corresponds to an
integrated luminosity of 9.4 fb(-1) collected by the
Collider Detector at Fermilab. We select events consistent
with the s-channel process including two jets and one
leptonically decaying W boson. The observed significance is
3.8 standard deviations with respect to the background-only
prediction. Assuming a top-quark mass of 172.5 GeV/c(2), we
measure the s-channel cross section to be 1.41(-0.42)(+0.44)
pb.},
Doi = {10.1103/physrevlett.112.231804},
Key = {fds308268}
}
@article{fds308417,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt,
N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zucchelli, S and CDF Collaboration},
Title = {Evidence for the charmless annihilation decay mode
B(s)(0)→π(+)π(-).},
Journal = {Physical review letters},
Volume = {108},
Number = {21},
Pages = {211803},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.211803},
Abstract = {We search for annihilation decay modes of neutral b mesons
into pairs of charmless charged hadrons with the upgraded
Collider Detector at the Fermilab Tevatron. Using a data
sample corresponding to 6 fb(-1) of integrated luminosity,
we obtain the first evidence for the B(s)(0)→π(+)π(-)
decay, with a significance of 3.7σ, and a measured
branching ratio B(B(s)(0)→π(+)π(-))=(0.57±0.15(stat)±0.10(syst))×10(-6).
A search for the B(0)→K(+)K(-) mode in the same sample
yields a significance of 2.0σ, and a central value estimate
B(B(0)→K(+)K(-))=(0.23±0.10(stat)±0.10(syst))×10(-6).},
Doi = {10.1103/physrevlett.108.211803},
Key = {fds308417}
}
@article{fds308671,
Author = {Acosta, and D, and others},
Title = {Evidence for the exclusive decay B/c+- --> J/psi pi+- and
measurement of the mass of the B/c meson},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {8},
Pages = {082002},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.082002},
Abstract = {We report first evidence for a fully reconstructed decay
mode of the B+/-_c meson in the channel B+/-_c --> J/psi
pi++/-, with J/psi --> mu+ mu-. The analysis is based on an
integrated luminosity of 360 pb-1 in p anti-p collisions at
1.96 TeV center of mass energy collected by the Collider
Detector at Fermilab. We observe 14.6 +/- 4.6 signal events
with a background of 7.1 +/- 0.9 events, and a fit to the
J/psi pi++/- mass spectrum yields a B+/-_c mass of 6285.7
+/- 5.3 (stat) +/- 1.2 (syst) MeV/c2. The probability of a
peak of this magnitude occurring by random fluctuation in
the search region is estimated as 0.012\%.},
Doi = {10.1103/physrevlett.96.082002},
Key = {fds308671}
}
@article{fds375881,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye,
T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja,
S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Artoni,
G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal,
D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barel, MZ and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann,
E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhalla, NK and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borissov, G and Bortoletto,
D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans,
G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey,
PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev, AR and Cabrera Urbán and S and Cadamuro,
L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace,
N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty,
D and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili,
B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ},
Title = {Evidence for the Higgs Boson Decay to a Z Boson and a Photon
at the LHC.},
Journal = {Physical review letters},
Volume = {132},
Number = {2},
Pages = {021803},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.132.021803},
Abstract = {The first evidence for the Higgs boson decay to a Z boson
and a photon is presented, with a statistical significance
of 3.4 standard deviations. The result is derived from a
combined analysis of the searches performed by the ATLAS and
CMS Collaborations with proton-proton collision datasets
collected at the CERN Large Hadron Collider (LHC) from 2015
to 2018. These correspond to integrated luminosities of
around 140 fb^{-1} for each experiment, at a
center-of-mass energy of 13 TeV. The measured signal yield
is 2.2±0.7 times the standard model prediction, and agrees
with the theoretical expectation within 1.9 standard
deviations.},
Doi = {10.1103/physrevlett.132.021803},
Key = {fds375881}
}
@article{fds321260,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H},
Title = {Evidence for the Higgs-boson Yukawa coupling to tau leptons
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {4},
Pages = {1-74},
Publisher = {Springer Nature},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2015)117},
Abstract = {Abstract: Results of a search for H → ττ decays are
presented, based on the full set of proton-proton collision
data recorded by the ATLAS experiment at the LHC during 2011
and 2012. The data correspond to integrated luminosities of
4.5 fb−1 and 20.3 fb−1 at centre-of-mass energies of
√s = 7 TeV and √s = 8 TeV respectively. All combinations
of leptonic (τ→ℓνν¯ with ℓ = e, μ) and hadronic
(τ → hadrons ν) tau decays are considered. An excess of
events over the expected background from other Standard
Model processes is found with an observed (expected)
significance of 4.5 (3.4) standard deviations. This excess
provides evidence for the direct coupling of the recently
discovered Higgs boson to fermions. The measured signal
strength, normalised to the Standard Model expectation, of
μ = 1. 43− 0.37+ 0.43 is consistent with the predicted
Yukawa coupling strength in the Standard Model.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP04(2015)117},
Key = {fds321260}
}
@article{fds308318,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and AbdelKhalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and AlconadaVerzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and AlvarezGonzalez, B and Alviggi, MG and Amako, K and AmaralCoutinho, Y and Amelung, C and Ammosov, VV and AmorDosSantos, SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and AperioBella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
M},
Title = {Evidence for the spin-0 nature of the Higgs boson using
ATLAS data},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {726},
Number = {1-3},
Pages = {120-144},
Publisher = {Elsevier BV},
Year = {2013},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2013.08.026},
Abstract = {Studies of the spin and parity quantum numbers of the Higgs
boson are presented, based on proton-proton collision data
collected by the ATLAS experiment at the LHC. The Standard
Model spin-parity JP=0+ hypothesis is compared with
alternative hypotheses using the Higgs boson decays
H→γγ, H→ZZ*→4ℓ and H→WW*→ℓνℓν, as well
as the combination of these channels. The analysed dataset
corresponds to an integrated luminosity of 20.7 fb-1
collected at a centre-of-mass energy of s=8TeV. For the
H→ZZ*→4ℓ decay mode the dataset corresponding to an
integrated luminosity of 4.6 fb-1 collected at s=7TeV is
included. The data are compatible with the Standard Model
JP=0+ quantum numbers for the Higgs boson, whereas all
alternative hypotheses studied in this Letter, namely some
specific JP=0-, 1+, 1-, 2+ models, are excluded at
confidence levels above 97.8%. This exclusion holds
independently of the assumptions on the coupling strengths
to the Standard Model particles and in the case of the JP=2+
model, of the relative fractions of gluon-fusion and
quark-antiquark production of the spin-2 particle. The data
thus provide evidence for the spin-0 nature of the Higgs
boson, with positive parity being strongly preferred. ©
2013 CERN.},
Doi = {10.1016/j.physletb.2013.08.026},
Key = {fds308318}
}
@article{fds308914,
Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Auchincloss, P and Austern, M and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bolognesi, V and Bortoletto, D and Boswell,
C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman, J and Cheng, M},
Title = {Evidence for top quark production in p-barp collisions at
sqrt s =1.8 TeV.},
Journal = {Physical review letters},
Volume = {73},
Number = {2},
Pages = {225-231},
Publisher = {American Physical Society (APS)},
Year = {1994},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.73.225},
Abstract = {We summarize a search for the top quark with the Collider
Detector at Fermilab (CDF) in a sample of p̄p collisions at
s =1.8 TeV with an integrated luminosity of 19.3 pb-1. We
find 12 events consistent with either two W bosons, or a W
boson and at least one b jet. The probability that the
measured yield is consistent with the background is 0.26%.
Though the statistics are too limited to establish firmly
the existence of the top quark, a natural interpretation of
the excess is that it is due to tt̄ production. Under this
assumption, constrained fits to individual events yield a
top quark mass of 174±10-12+13 GeV/c2. The tt̄ production
cross section is measured to be 13.9-4.8+6.1 pb. © 1994 The
American Physical Society.},
Doi = {10.1103/physrevlett.73.225},
Key = {fds308914}
}
@article{fds308915,
Author = {al, FAE},
Title = {Evidence for top-quark production in (p)over-bar-p
collisions at root-s=1.8 tev},
Journal = {Phys. Rev. D},
Volume = {50},
Number = {5},
Pages = {2966-3026},
Publisher = {American Physical Society (APS)},
Year = {1994},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevd.50.2966},
Abstract = {© 1994 The American Physical Society. We present the
results of a search for the top quark in 19.3 pb-1 of p̄p
collisions at s =1.8 TeV. The data were collected at the
Fermilab Tevatron collider using the Collider Detector at
Fermilab (CDF). The search includes standard model tt̄
decays to final states eeνν̄, eμνν̄, and μμνν̄
as well as e+ν+jets or μ+ν+jets. In the (e,μ)+ν+jets
channel we search for b quarks from t decays via secondary
vertex identification and via semileptonic decays of the b
and cascade c quarks. In the dilepton final states we find
two events with a background of 0.56-0.13+0.25 events. In
the e,μ+ν+jets channel with a b identified via a secondary
vertex, we find six events with a background of 2.3±0.3.
With a b identified via a semileptonic decay, we find seven
events with a background of 3.1±0.3. The secondary vertex
and semileptonic-decay samples have three events in common.
The probability that the observed yield is consistent with
the background is estimated to be 0.26%. The statistics are
too limited to firmly establish the existence of the top
quark; however, a natural interpretation of the excess is
that it is due to tt̄ production. We present several
cross-checks. Some support this hypothesis; others do not.
Under the assumption that the excess yield over background
is due to tt̄, constrained fitting on a subset of the
events yields a mass of 174±10-12+13 GeV/c2 for the top
quark. The tt̄ cross section, using this top quark mass to
compute the acceptance, is measured to be 13.9-4.8+6.1
pb.},
Doi = {10.1103/physrevd.50.2966},
Key = {fds308915}
}
@article{fds365423,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler,
A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso,
S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Evidence for tt¯ tt¯ production in the multilepton final
state in proton–proton collisions at √s=13 TeV with the
ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {11},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08509-3},
Abstract = {A search is presented for four-top-quark production using an
integrated luminosity of 139 fb- 1 of proton–proton
collision data at a centre-of-mass energy of 13TeV collected
by the ATLAS detector at the LHC. Events are selected if
they contain a same-sign lepton pair or at least three
leptons (electrons or muons). Jet multiplicity, jet flavour
and event kinematics are used to separate signal from the
background through a multivariate discriminant, and
dedicated control regions are used to constrain the dominant
backgrounds. The four-top-quark production cross section is
measured to be 24-6+7 fb. This corresponds to an observed
(expected) significance with respect to the background-only
hypothesis of 4.3 (2.4) standard deviations and provides
evidence for this process.},
Doi = {10.1140/epjc/s10052-020-08509-3},
Key = {fds365423}
}
@article{fds337203,
Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
J and Thompson, GA and Thomson, E and Tipton, P and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán,
J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka,
J},
Title = {Evidence for tt̄γ production and measurement of
σtt̄γ/σtt̄},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {84},
Number = {3},
Year = {2011},
url = {http://dx.doi.org/10.1103/PhysRevD.84.031104},
Abstract = {Using data corresponding to 6.0fb-1 of pp̄ collisions at
√s=1.96TeV collected by the CDF II detector, we present a
cross section measurement of top-quark pair production with
an additional radiated photon in the central region with 10
GeV or more of transverse energy tt̄γ. The events are
selected by looking for a lepton (ℓ or μ), a photon (γ),
significant transverse momentum imbalance (ET), large total
transverse energy, and three or more jets, with at least one
identified as containing a b quark (b). Using an event
selection optimized for the tt̄γ candidate sample, we also
measure the cross section of tt̄ (σtt̄). We measure the
tt̄γ cross section (σtt̄γ) to be 0.18±0.08pb, and the
ratio of σtt̄γ to σtt̄ to be 0.024±0.009. We observe a
probability of 0.0015 (3.0 standard deviations) of the
background (non-tt̄γ events alone producing 30 events or
more. © 2011 American Physical Society.},
Doi = {10.1103/PhysRevD.84.031104},
Key = {fds337203}
}
@article{fds330943,
Author = {al, FAE},
Title = {Evidence for W+W- production in (p)over-bar-p collisions at
root s=1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {78},
Number = {24},
Pages = {4536-4540},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevLett.78.4536},
Abstract = {We present results of a search for W+W− production through
the leptonic decay channel W+W− → l+l− in vv⊯ in
p⊯p collisions at √s = 1.8TeV. In a 108pb−1 data
sample recorded with the Collider Detector at Fermilab, five
W+W− candidates are found with an expected standard model
background of 1.2±0.3events. The W+W− production cross
section is measured to beσ(p⊯p → W+W−)=10.2−5.1+6.3(stat)±1.6(syst)pb,
in agreement with the standard model prediction. Limits on
WWγand WWZ anomalous couplings are presented. © 1997
American Physical Society.},
Doi = {10.1103/PhysRevLett.78.4536},
Key = {fds330943}
}
@article{fds375892,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH},
Title = {Evidence of off-shell Higgs boson production from ZZ
leptonic decay channels and constraints on its total width
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {846},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138223},
Abstract = {This Letter reports on a search for off-shell production of
the Higgs boson using 139 fb−1 of pp collision data at s=
13 TeV collected by the ATLAS detector at the Large Hadron
Collider. The signature is a pair of Z bosons, with
contributions from both the production and subsequent decay
of a virtual Higgs boson and the interference of that
process with other processes. The two observable final
states are ZZ→4ℓ and ZZ→2ℓ2ν with ℓ=e or μ. In
the ZZ→4ℓ final state, a dense Neural Network is used to
enhance analysis sensitivity with respect to matrix
element-based discrimination. The background-only hypothesis
is rejected with an observed (expected) significance of 3.3
(2.2) standard deviations, representing experimental
evidence for off-shell Higgs boson production. Assuming that
no new particles enter the production of the virtual Higgs
boson, its total width can be deduced from the measurement
of its off-shell production cross-section. The measured
total width of the Higgs boson is 4.5−2.5+3.3 MeV, and the
observed (expected) upper limit on the total width is found
to be 10.5 (10.9) MeV at 95% confidence level.},
Doi = {10.1016/j.physletb.2023.138223},
Key = {fds375892}
}
@article{fds321238,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo,
T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell,
SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Evidence of Wγγ Production in pp Collisions at
sqrt[s]=8 TeV and Limits on Anomalous Quartic Gauge
Couplings with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {115},
Number = {3},
Pages = {031802},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.115.031802},
Abstract = {This Letter reports evidence of triple gauge boson
production pp→W(ℓν)γγ+X, which is accessible for the
first time with the 8 TeV LHC data set. The fiducial cross
section for this process is measured in a data sample
corresponding to an integrated luminosity of
20.3 fb^{-1}, collected by the ATLAS detector in 2012.
Events are selected using the W boson decay to eν or μν
as well as requiring two isolated photons. The measured
cross section is used to set limits on anomalous quartic
gauge couplings in the high diphoton mass
region.},
Doi = {10.1103/physrevlett.115.031802},
Key = {fds321238}
}
@article{fds308472,
Author = {Aaltonen, and T, and others},
Title = {Exclusion of an Exotic Top Quark with -4/3 Electric Charge
Using Soft Lepton Tagging},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {10},
Pages = {101801},
Publisher = {American Physical Society},
Year = {2010},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.101801},
Abstract = {We present a measurement of the electric charge of the top
quark using pp collisions corresponding to an integrated
luminosity of 2.7 fb(-1) at the CDF II detector. We
reconstruct tt events in the lepton + jets final state. We
use soft lepton taggers to determine the flavor of the b
jets, which we use to reconstruct the top quark's electric
charge and exclude an exotic top quark with -4/3 charge at
95% confidence level. This is the strongest exclusion of the
exotic charge scenario and the first to use soft leptons for
this purpose.},
Doi = {10.1103/PhysRevLett.105.101801},
Key = {fds308472}
}
@article{fds308320,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar,
R},
Title = {Exclusion of exotic top-like quarks with -4/3 electric
charge using jet-charge tagging in single-lepton tt̄ events
at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {3},
Pages = {032003},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.88.032003},
Abstract = {We report on a measurement of the top-quark electric charge
in tt̄ events in which one W boson originating from the
top-quark pair decays into leptons and the other into
hadrons. The event sample was collected by the CDF II
detector in √s=1.96 TeV proton-antiproton collisions and
corresponds to 5.6 fb-1. We find the data to be consistent
with the standard model and exclude the existence of an
exotic quark with -4/3 electric charge and mass of the
conventional top quark at the 99% confidence level. © 2013
American Physical Society.},
Doi = {10.1103/PhysRevD.88.032003},
Key = {fds308320}
}
@article{fds375894,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Fast b-tagging at the high-level trigger of the ATLAS
experiment in LHC Run 3},
Journal = {Journal of Instrumentation},
Volume = {18},
Number = {11},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1088/1748-0221/18/11/P11006},
Abstract = {The ATLAS experiment relies on real-time hadronic jet
reconstruction and b-tagging to record fully hadronic events
containing b-jets. These algorithms require track
reconstruction, which is computationally expensive and could
overwhelm the high-level-trigger farm, even at the reduced
event rate that passes the ATLAS first stage hardware-based
trigger. In LHC Run 3, ATLAS has mitigated these
computational demands by introducing a fast
neural-network-based b-tagger, which acts as a low-precision
filter using input from hadronic jets and tracks. It runs
after a hardware trigger and before the remaining
high-level-trigger reconstruction. This design relies on the
negligible cost of neural-network inference as compared to
track reconstruction, and the cost reduction from limiting
tracking to specific regions of the detector. In the case of
Standard Model HH → bb̄bb̄, a key signature relying on
b-jet triggers, the filter lowers the input rate to the
remaining high-level trigger by a factor of five at the
small cost of reducing the overall signal efficiency by
roughly 2%.},
Doi = {10.1088/1748-0221/18/11/P11006},
Key = {fds375894}
}
@article{fds321353,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H},
Title = {Fiducial and differential cross sections of Higgs boson
production measured in the four-lepton decay channel in pp
collisions at √s=8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {738},
Pages = {234-253},
Publisher = {Elsevier BV},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2014.09.054},
Abstract = {Measurements of fiducial and differential cross sections of
Higgs boson production in the H→ZZ*→4ℓ decay channel
are presented. The cross sections are determined within a
fiducial phase space and corrected for detection efficiency
and resolution effects. They are based on 20.3fb-1 of pp
collision data, produced at √s=8 TeV centre-of-mass energy
at the LHC and recorded by the ATLAS detector. The
differential measurements are performed in bins of
transverse momentum and rapidity of the four-lepton system,
the invariant mass of the subleading lepton pair and the
decay angle of the leading lepton pair with respect to the
beam line in the four-lepton rest frame, as well as the
number of jets and the transverse momentum of the leading
jet. The measured cross sections are compared to selected
theoretical calculations of the Standard Model expectations.
No significant deviation from any of the tested predictions
is found.},
Doi = {10.1016/j.physletb.2014.09.054},
Key = {fds321353}
}
@article{fds308436,
Author = {Aaltonen, and T, and al, E},
Title = {First Measurement of the Angular Coefficients of {Drell-Yan}
${e}^{+}{e}^{-}$ Pairs in the ${Z}$ Mass Region from
$p\overline{p}$ Collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {24},
Pages = {241801},
Publisher = {American Physical Society},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.241801},
Abstract = {We report on the first measurement of the angular
distributions of final state electrons in pp¯ → γ*/Z →
e(+)e(-) + X events produced in the Z boson mass region at
√s1.96 TeV. The data sample collected by the CDF II
detector for this result corresponds to 2.1 fb(-1) of
integrated luminosity. The angular distributions are studied
as a function of the transverse momentum of the
electron-positron pair and show good agreement with the
Lam-Tung relation, consistent with a spin-1 description of
the gluon, and demonstrate that, at high values of the
transverse momentum, Z bosons are produced via
quark-antiquark annihilation and quark-gluon Compton
processes.},
Doi = {10.1103/PhysRevLett.106.241801},
Key = {fds308436}
}
@article{fds308480,
Author = {Aaltonen, and T, and others},
Title = {First Measurement of the b-jet Cross Section in Events with
a $W$ Boson in $p \bar{p}$ Collisions at $\sqrt{s} = 1.96$
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {13},
Pages = {131801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.131801},
Abstract = {http://arxiv.org/abs/0909.1505},
Doi = {10.1103/PhysRevLett.104.131801},
Key = {fds308480}
}
@article{fds321230,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {First measurement of the forward-backward asymmetry in
bottom-quark pair production at high mass},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.92.032006},
Abstract = {We measure the particle-level forward-backward production
asymmetry in bb¯ pairs with masses (mbb¯) larger than 150
GeV/c2, using events with hadronic jets and employing jet
charge to distinguish b from b¯. The measurement uses 9.5
fb-1 of pp¯ collisions at a center-of-mass energy of 1.96
TeV recorded by the CDF II detector. The asymmetry as a
function of mbb¯ is consistent with zero, as well as with
the predictions of the standard model. The measurement
disfavors a simple model including an axigluon with a mass
of 200 GeV/c2, whereas a model containing a heavier 345
GeV/c2 axigluon is not excluded.},
Doi = {10.1103/PhysRevD.92.032006},
Key = {fds321230}
}
@article{fds308608,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
Title = {First measurement of the fraction of top-quark pair
production through gluon-gluon fusion},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {78},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2008},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.78.111101},
Abstract = {We present the first measurement of σ(gg→tt̄)/
σ(pp̄→tt̄). We use 0.96fb-1 of s=1.96TeV pp̄ collision
data recorded with the CDF II detector at Fermilab. Using
charged particles with low transverse momentum in tt̄
events, we find σ(gg→ tt̄)/σ(pp̄→tt̄)=0.07±0.14(stat)±0.
07(syst), corresponding to a 95% confidence level upper
limit of 0.33, in agreement with the standard model
next-to-leading-order prediction of 0.15±0.05. © 2008 The
American Physical Society.},
Doi = {10.1103/PhysRevD.78.111101},
Key = {fds308608}
}
@article{fds308475,
Author = {Aaltonen, and T, and others},
Title = {First Measurement of the Ratio $\sigma_{(t\bar{t})} /
\sigma_{(Z/\gamma^*\to ll)}$ and Precise Extraction of the
$t\bar{t}$ Cross Section},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {1},
Pages = {012001},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.012001},
Abstract = {http://arxiv.org/abs/1004.3224},
Doi = {10.1103/PhysRevLett.105.012001},
Key = {fds308475}
}
@article{fds308543,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini,
J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin,
M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, BY and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo,
KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin,
PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen,
AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer,
MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino,
G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt,
MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider,
FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas,
J},
Title = {First measurement of the ratio of branching fractions B(Λb
0→Λc+μ-ν̄μ)/B(Λb 0→Λc+π-)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2009},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.79.032001},
Abstract = {This article presents the first measurement of the ratio of
branching fractions B(Λb0→Λc+μ-ν̄μ)/
B(Λb0→Λc+π-). Measurements in two control samples using
the same technique B(B̄0→D+μ- ν̄μ)/B(B̄0→D+π-)
and B(B̄ 0→D*(2010)+μ-ν̄μ)/ B(B̄0→D*(2010)+π-)
are also reported. The analysis uses data from an integrated
luminosity of approximately 172pb-1 of pp̄ collisions at
s=1.96TeV, collected with the CDF II detector at the
Fermilab Tevatron. The relative branching fractions are
measured to be B(Λb 0→Λc+μ-ν̄μ)B(Λb
0→Λc+π-)=16.6±3.0(stat) ±1.0(syst)+2.6-3.4(PDG)
±0.3(EBR), B(B̄0→D+μ-ν̄μ) B(B̄0→D+π-)=9.9±1.0(stat)
±0.6(syst)±0.4(PDG)± 0.5(EBR), and B(B̄0→D*(
2010)+μ-ν̄μ)B(B̄0→D*( 2010)+π-)=16.5±2.3(stat)
±0.6(syst)±0.5(PDG)± 0.8(EBR). The uncertainties are from
statistics (stat), internal systematics (syst), world
averages of measurements published by the Particle Data
Group or subsidiary measurements in this analysis (PDG), and
unmeasured branching fractions estimated from theory (EBR),
respectively. This article also presents measurements of the
branching fractions of four new Λb 0 semileptonic decays:
Λb0→Λc( 2595)+μ-ν̄μ, Λb0→Λc( 2625)+μ-ν̄μ,
Λb0→Σc( 2455)0π+μ-ν̄μ, and Λb 0→Σc(2455)++π-μ-ν̄μ,
relative to the branching fraction of the Λb0→Λc+μ-
ν̄μ decay. Finally, the transverse-momentum distribution
of Λb0 baryons produced in pp̄ collisions is measured and
found to be significantly different from that of B̄0
mesons, which results in a modification in the production
cross-section ratio σΛb0/σB̄0 with respect to the CDF I
measurement. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevD.79.032001},
Key = {fds308543}
}
@article{fds308626,
Author = {Abulencia, and A, and others},
Title = {First Measurement of the Ratio of Central-Electron to
Forward-Electron W Partial Cross Sections in p-pbar
Collisions at sqrt{s} = 1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {25},
Pages = {251801},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.251801},
Abstract = {We present a measurement of sigma(p[overline
p]-->W){\AA}~[script B](W-->enu) at sqrt(s)=1.96 TeV, using
electrons identified in the forward region
(1.2-90+95(syst)$\pm$162(lum) pb. Combining this result with
a previous CDF measurement obtained using electrons in the
central region (|eta|},
Doi = {10.1103/physrevlett.98.251801},
Key = {fds308626}
}
@article{fds361224,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and González, BÁ and Amerio,
S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini,
J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin,
M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, BY and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens,
P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao,
T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer,
MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Palencia,
E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks,
B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus,
C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt,
M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber,
I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer,
B},
Title = {First measurement of the tt̄ differential cross section
dσ/dMtt̄ in pp̄ collisions at s=1.96TeV},
Journal = {Physical Review Letters},
Volume = {102},
Number = {22},
Pages = {222003},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevLett.102.222003},
Abstract = {We present a measurement of the tt̄ differential cross
section with respect to the tt̄ invariant mass, dσ/dMtt̄,
in pp̄ collisions at s=1.96TeV using an integrated
luminosity of 2.7fb-1 collected by the CDF II experiment.
The tt̄ invariant mass spectrum is sensitive to a variety
of exotic particles decaying into tt̄ pairs. The result is
consistent with the standard model expectation, as modeled
by PYTHIA with CTEQ5L parton distribution functions. © 2009
The American Physical Society.},
Doi = {10.1103/PhysRevLett.102.222003},
Key = {fds361224}
}
@article{fds308623,
Author = {Aaltonen, and T, and others},
Title = {First Measurement of the W Boson Mass in Run II of the
Tevatron},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {15},
Pages = {151801},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.151801},
Abstract = {We present a measurement of the W-boson mass using 200 pb-1
of data collected in p[overline p] collisions at
sqrt(s)=1.96 TeV by the CDF II detector at run II of the
Fermilab Tevatron. With a sample of 63 964 W-->enu
candidates and 51 128 W-->µnu candidates, we measure MW=80
413$\pm$34stat$\pm$34syst=80 413$\pm$48 MeV/c2. This is the
most precise single measurement of the W-boson mass to
date.},
Doi = {10.1103/physrevlett.99.151801},
Key = {fds308623}
}
@article{fds308588,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and De
Lorenzo, G and Dell'Orso, M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di
Ruzza, B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt,
J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson,
W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Koay, SA and Kondo,
K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus,
J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci,
C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak,
R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Mangano, ML and Manousakis, A and Margaroli, F and Marino,
C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan Griso,
S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic,
V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó,
O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A},
Title = {First measurement of W boson production in association with
a single Charm quark in pp collisions at sqrt(s)=1.96
TeV.},
Journal = {Physical review letters},
Volume = {100},
Number = {9},
Pages = {091803},
Year = {2008},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.100.091803},
Abstract = {We present the first measurement of the production cross
section of a W boson with a single charm quark (c) in pp
collisions at sqrt(s)=1.96 TeV, using soft muon tagging of c
jets. In a data sample of approximately 1.8 fb(-1), recorded
with the Collider Detector at Fermilab II detector at the
Fermilab Tevatron, we select events with W+1 or 2 jets. We
use the charge correlation between the W and the muon from
the semileptonic decay of a charm hadron to extract the Wc
signal. We measure sigma Wc(PTc >20 GeV/c,|eta c|<1.5) x
BR(W-->l nu)=9.8+/-3.2 pb, in agreement with theoretical
expectations.},
Doi = {10.1103/physrevlett.100.091803},
Key = {fds308588}
}
@article{fds308704,
Author = {Acosta, and D, and others},
Title = {First measurements of inclusive W and Z cross sections from
Run II of the Tevatron collider},
Journal = {Phys. Rev. Lett.},
Volume = {94},
Number = {9},
Pages = {091803},
Year = {2005},
url = {http://dx.doi.org/10.1103/physrevlett.94.091803},
Abstract = {http://arxiv.org/abs/hep-ex/0406078},
Doi = {10.1103/physrevlett.94.091803},
Key = {fds308704}
}
@article{fds308514,
Author = {Aaltonen, T and others},
Title = {First Observation of B̅ s0→Ds ± K∓ and
Measurement of the Ratio of Branching Fractions B(B̅
s0→Ds ± K∓)/B(B̅ s0→Ds+π-)},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {19},
Pages = {191802},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.191802},
Abstract = {A combined mass and particle identification fit is used to
make the first observation of the decay B̅ s0→Ds ±
K∓ and measure the branching fraction of B̅ s0→Ds
± K∓ relative to B̅ s0→Ds+π-. This analysis
uses 1.2 fb-1 integrated luminosity of pp̅ collisions
at sqrt[s]=1.96 TeV collected with the CDF II detector
at the Fermilab Tevatron collider. We observe a B̅ s0→Ds
± K∓ signal with a statistical significance of
8.1σ and measure B(B̅ s0→Ds ± K∓)/B(B̅
s0→Ds+π-)=0.097 ± 0.018(stat) ±
0.009(syst).},
Doi = {10.1103/physrevlett.103.191802},
Key = {fds308514}
}
@article{fds308859,
Author = {al, FAE},
Title = {First observation of the all-hadronic decay of t(t)over-bar
pairs},
Journal = {Phys. Rev. Lett.},
Volume = {79},
Number = {11},
Pages = {1992-1997},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.1992},
Abstract = {We present the first observation of the all hadronic decay
of tt― pairs. The analysis is performed using 109 pb−1
of pp― collisions at s = 1.8 TeV collected with the
Collider Detector at Fermilab. We observe an excess of
events with five or more jets, including one or two b jets,
relative to background expectations. Based on this excess we
evaluate the production cross section to be in agreement
with previous results. We measure the top mass to be
186±10±12 GeV/c2. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.79.1992},
Key = {fds308859}
}
@article{fds308518,
Author = {Aaltonen, T and others},
Title = {First Observation of Vector Boson Pairs in a Hadronic Final
State at the Tevatron Collider},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {9},
Pages = {091803},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.091803},
Abstract = {We present the first observation in hadronic collisions of
the electroweak production of vector boson pairs (VV, V=W,
Z) where one boson decays to a dijet final state. The data
correspond to 3.5 fb-1 of integrated luminosity of pp̅
collisions at sqrt[s]=1.96 TeV collected by the CDF II
detector at the Fermilab Tevatron. We observe 1516 ±
239(stat) ± 144(syst) diboson candidate events and
measure a cross section σ(pp̅ →VV+X) of 18.0 ±
2.8(stat) ± 2.4(syst) ± 1.1(lumi) pb, in
agreement with the expectations of the standard
model.},
Doi = {10.1103/physrevlett.103.091803},
Key = {fds308518}
}
@article{fds308596,
Author = {Aaltonen, T and Abulencia, A and Adelman, J and Akimoto, T and Albrow,
MG and Álvarez González, B and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa,
T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli,
F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci,
MA},
Title = {First run II measurement of the W boson mass at the Fermilab
Tevatron},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {77},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2008},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.77.112001},
Abstract = {We describe a measurement of the W boson mass mW using
200pb-1 of s=1.96TeV pp̄ collision data taken with the CDF
II detector. With a sample of 63964 W→eν candidates and
51128 W→μν candidates, we measure mW=[80.413±0.034(stat)±0.034(sys)=80.413±0.048]GeV/c2.
This is the single most precise mW measurement to date. When
combined with other measured electroweak parameters, this
result further constrains the properties of new unobserved
particles coupling to W and Z bosons. © 2008 The American
Physical Society.},
Doi = {10.1103/PhysRevD.77.112001},
Key = {fds308596}
}
@article{fds308284,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester Iii and WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {First search for exotic Z Boson decays into photons and
neutral pions in hadron collisions.},
Journal = {Physical review letters},
Volume = {112},
Number = {11},
Pages = {111803},
Year = {2014},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.112.111803},
Abstract = {A search for forbidden and exotic Z boson decays in the
diphoton mass spectrum is presented for the first time in
hadron collisions, based on data corresponding to 10.0
fb(-1) of integrated luminosity from proton-antiproton
collisions at √s = 1.96 TeV collected by the CDF
experiment. No evidence of signal is observed, and 95%
credibility level Bayesian upper limits are set on the
branching ratios of decays of the Z boson to a photon and
neutral pion (which is detected as a photon), a pair of
photons, and a pair of neutral pions. The observed branching
ratio limits are 2.01 × 10(-5) for Z → π(0)γ, 1.46 ×
10(-5) for Z → γγ, and 1.52 × 10(-5) for Z →
π(0)π(0). The Z → π(0)γ and Z → γγ limits improve
the most stringent results from other experiments by factors
of 2.6 and 3.6, respectively. The Z → π(0)π(0) branching
ratio limit is the first experimental result on this
decay.},
Doi = {10.1103/physrevlett.112.111803},
Key = {fds308284}
}
@article{fds308434,
Author = {Aaltonen, and T, and al, E},
Title = {First Search for Multijet Resonances in $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$
$p\overline{p}$ Collisions},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {4},
Pages = {042001},
Publisher = {American Physical Society},
Year = {2011},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.042001},
Abstract = {We present the first model independent search for three-jet
hadronic resonances within multijet events in sqrt(s) =
1.96 TeV pp collisions at the Fermilab Tevatron using
the CDF II detector. Pair production of supersymmetric
gluinos and squarks with hadronic R-parity violating decays
is employed as an example of a new physics benchmark for
this signature. Selection criteria based on the kinematic
properties of an ensemble of jet combinations within each
event help to extract signal from copious QCD background. No
significant excess outside the top quark mass window is
observed in data with an integrated luminosity of
3.2 fb(-1). We place 95% confidence level limits on the
production cross section σ(pp → XX')×BR(gg →
3 jet + 3 jet) where X, X' = g, q, or q, with q, q
→ g + jet, as a function of gluino mass, in the range of
77 GeV/c2 to 240 GeV/c2.},
Doi = {10.1103/PhysRevLett.107.042001},
Key = {fds308434}
}
@article{fds308546,
Author = {Aaltonen, T and others},
Title = {First simultaneous measurement of the top quark mass in the
lepton + jets and dilepton channels at CDF},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {9},
Pages = {092005},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.092005},
Abstract = {We present a measurement of the mass of the top quark using
data corresponding to an integrated luminosity of 1.9fb-1 of
pp̄ collisions collected at s=1.96TeV with the CDF II
detector at Fermilab's Tevatron. This is the first
measurement of the top quark mass using top-antitop pair
candidate events in the lepton+jets and dilepton decay
channels simultaneously. We reconstruct two observables in
each channel and use a nonparametric kernel density
estimation technique to derive two-dimensional probability
density functions from simulated signal and background
samples. The observables are the top quark mass and the
invariant mass of two jets from the W decay in the
lepton+jets channel, and the top quark mass and the scalar
sum of transverse energy of the event in the dilepton
channel. We perform a simultaneous fit for the top quark
mass and the jet energy scale, which is constrained in situ
by the hadronic W boson mass. Using 332 lepton+jets
candidate events and 144 dilepton candidate events, we
measure the top quark mass to be Mtop=171.9±1.
7(stat+JES)±1.1(othersyst)GeV/c2=171.9±2.0GeV/c2. © 2009
The American Physical Society.},
Doi = {10.1103/PhysRevD.79.092005},
Key = {fds308546}
}
@article{fds321332,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ},
Title = {Flavor tagged time-dependent angular analysis of the Bs0
→J/ψφ decay and extraction of ΔΓs and the weak phase
φs in ATLAS},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.90.052007},
Abstract = {A measurement of the Bs0→J/ψφ decay parameters, updated
to include flavor tagging is reported using 4.9fb-1 of
integrated luminosity collected by the ATLAS detector from
s=7TeV pp collisions recorded in 2011 at the LHC. The values
measured for the physical parameters are
φs=0.12±0.25(stat)±0.05(syst)radΔΓs=0.053±0.021(stat)±0.010(syst)ps-1Γs=0.677±0.007(stat)±0.004(syst)ps-1|A
(0)|2=0.220±0.008(stat)±0.009(syst)|A0(0)|2=0.529±0.006(stat)±0.012(syst)δ=3.89±0.47(stat)±0.11(syst)radwhere
the parameter ΔΓs is constrained to be positive. The
S-wave contribution was measured and found to be compatible
with zero. Results for φs and ΔΓs are also presented as
68% and 95% likelihood contours, which show agreement with
the Standard Model expectations.},
Doi = {10.1103/PhysRevD.90.052007},
Key = {fds321332}
}
@article{fds308882,
Author = {al, FAE},
Title = {Forward-backward charge asymmetry of electron Paris above
the Z(0) pole},
Journal = {Phys. Rev. Lett.},
Volume = {77},
Number = {13},
Pages = {2616-2621},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevLett.77.2616},
Abstract = {We present a measurement of the forward-backward charge
asymmetry of the process pp¯ → Z0/γ + X, Z0/γ →
e+e− at Mee > MZ using 110 pb−1 of data at √ s = 1.8
TeV collected at the Collider Detector at Fermilab. The
measured charge asymmetries are 0.43 ± 0.10 in the
invariant mass region Mee > 105 GeV/c2, and 0.070 ± 0.016
in the region 75 < Mee < 105 GeV/c2. These results are
consistent with the standard model values of 0.528 ± 0.009
and 0.052 ± 0.002, respectively. © 1996 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.77.2616},
Key = {fds308882}
}
@article{fds308878,
Author = {al, FAE},
Title = {Further properties of high-mass multijet events at the
Fermilab proton-antiproton collider},
Journal = {Phys. Rev. D},
Volume = {54},
Number = {7},
Pages = {4221-4233},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevd.54.4221},
Abstract = {The properties of high-mass multijet events produced at the
Fermilab proton-antiproton collider are compared with
leading order QCD matrix element predictions, QCD parton
shower Monte Carlo predictions, and the predictions from a
model in which events are distributed uniformly over the
available multibody phase space. Multijet distributions
corresponding to ([Formula presented]) variables that span
the [Formula presented]-body parameter space are found to be
well described by the QCD calculations for inclusive
three-jet, four-jet, and five-jet events. The agreement
between data, QCD matrix element calculations, and QCD
parton shower Monte Carlo predictions suggests that 2→2
scattering plus gluon radiation provides a good first
approximation to the full LO QCD matrix element for events
with three, four, or even five jets in the final state. ©
1996 The American Physical Society.},
Doi = {10.1103/physrevd.54.4221},
Key = {fds308878}
}
@article{fds327374,
Author = {Mindur, B and Åkesson, TPA and Anghinolfi, F and Antonov, A and Arslan,
O and Baker, OK and Banas, E and Bault, C and Beddall, AJ and Bendotti, J and Benjamin, DP and Bertelsen, H and Bingul, A and Bocci, A and Boldyrev,
AS and Brock, I and Capeáns Garrido and M and Catinaccio, A and Celebi, E and Cetin, SA and Choi, K and Dam, M and Danielsson, H and Davis, D and Degeorge, C and Derendarz, D and Desch, K and Di Girolamo and B and Dittus,
F and Dixon, N and Dressnandt, N and Dubinin, FA and Evans, H and Farthouat, P and Fedin, OL and Froidevaux, D and Gavrilenko, IL and Gay,
C and Gecse, Z and Godlewski, J and Grefe, C and Gurbuz, S and Hajduk, Z and Hance, M and Haney, B and Hansen, JB and Hansen, PH and Hawkins, AD and Heim, S and Holway, K and Kantserov, VA and Katounine, S and Kayumov, F and Keener, PT and Kisielewski, B and Klopov, NV and Konovalov, SP and Koperny, S and Korotkova, NA and Kowalski, TZ and Kramarenko, V and Krasnopevtsev, D and Kruse, M and Kudin, LG and Lichard, P and Loginov,
A and Lorenzo Martinez and N and Lucotte, A and Luehring, F and Lytken, E and Maleev, VP and Maevskiy, AS and Manjarres Ramos and J and Mashinistov,
RY and Meyer, C and Mialkovski, V and Mistry, K and Mitsou, VA and Nadtochi, AV and Newcomer, FM and Novodvorski, EG and Ogren, H and Oh,
SH and Oleshko, SB and Olszowska, J and Ostrowicz, W and Palacino, G and Patrichev, S and Penwell, J and Perez-Gomez, F and Peshekhonov, VD and Røhne, O and Reilly, MB and Rembser, C and Ricken, O and Romaniouk, A and Rousseau, D and Ryjov, V and Sasmaz, U and Schaepe,
S},
Title = {Gas gain stabilisation in the ATLAS TRT detector},
Journal = {Journal of Instrumentation},
Volume = {11},
Number = {4},
Year = {2016},
Month = {April},
url = {http://dx.doi.org/10.1088/1748-0221/11/04/P04027},
Abstract = {The ATLAS (one of two general purpose detectors at the LHC)
Transition Radiation Tracker (TRT) is the outermost of the
three tracking subsystems of the ATLAS Inner Detector. It is
a large straw-based detector and contains about 350,000
electronics channels. The performance of the TRT as tracking
and particularly particle identification detector strongly
depends on stability of the operation parameters with most
important parameter being the gas gain which must be kept
constant across the detector volume. The gas gain in the
straws can vary significantly with atmospheric pressure,
temperature, and gas mixture composition changes. This paper
presents a concept of the gas gain stabilisation in the TRT
and describes in detail the Gas Gain Stabilisation System
(GGSS) integrated into the Detector Control System (DCS).
Operation stability of the GGSS during Run-1 is
demonstrated.},
Doi = {10.1088/1748-0221/11/04/P04027},
Key = {fds327374}
}
@article{fds308548,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Aurisano, A and Azfar, F and Azzurri, P and Badgett,
W and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung,
K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci,
MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway,
J},
Title = {Global search for new physics with 2.0fb-1 at
CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.79.011101},
Abstract = {Data collected in run II of the Fermilab Tevatron are
searched for indications of new electroweak-scale physics.
Rather than focusing on particular new physics scenarios,
CDF data are analyzed for discrepancies with the standard
model prediction. A model-independent approach (Vista)
considers gross features of the data, and is sensitive to
new large cross-section physics. Further sensitivity to new
physics is provided by two additional algorithms: a Bump
Hunter searches invariant mass distributions for "bumps"
that could indicate resonant production of new particles,
and the Sleuth procedure scans for data excesses at large
summed transverse momentum. This combined global search for
new physics in 2.0fb-1 of pp̄ collisions at s=1.96TeV
reveals no indication of physics beyond the standard model.
© 2009 The American Physical Society.},
Doi = {10.1103/PhysRevD.79.011101},
Key = {fds308548}
}
@article{fds308740,
Author = {Acosta, D and al, E},
Title = {Heavy flavor properties of jets produced in p anti-p
interactions at s**(1/2) = 1.8-TeV},
Journal = {Phys. Rev.},
Volume = {D69},
Number = {7},
Pages = {072004},
Publisher = {American Physical Society (APS)},
Year = {2004},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.69.072004},
Abstract = {We present a detailed examination of the heavy flavor
properties of jets produced at the Fermilab Tevatron
collider. The data set, collected with the Collider Detector
at Fermilab, consists of events with two or more jets with
transverse energy ET >= 15ÊGeV and pseudorapidity | eta | =
2ÊGeV/c) in the data to that in the tuned simulation. We
find that this rate is larger than what is expected for the
conventional production and semileptonic decay of pairs of
hadrons with heavy flavor.},
Doi = {10.1103/PhysRevD.69.072004},
Key = {fds308740}
}
@article{fds365426,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
C},
Title = {Higgs boson production cross-section measurements and their
EFT interpretation in the 4 ℓ decay channel at √s=
13 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8227-9},
Abstract = {Higgs boson properties are studied in the four-lepton decay
channel (where lepton = e, μ) using 139 fb - 1 of
proton–proton collision data recorded at s=13 TeV by the
ATLAS experiment at the Large Hadron Collider. The inclusive
cross-section times branching ratio for H→ ZZ∗ decay is
measured to be 1.34 ± 0.12 pb for a Higgs boson with
absolute rapidity below 2.5, in good agreement with the
Standard Model prediction of 1.33 ± 0.08 pb. Cross-sections
times branching ratio are measured for the main Higgs boson
production modes in several exclusive phase-space regions.
The measurements are interpreted in terms of coupling
modifiers and of the tensor structure of Higgs boson
interactions using an effective field theory approach.
Exclusion limits are set on the CP-even and CP-odd ‘beyond
the Standard Model’ couplings of the Higgs boson to vector
bosons, gluons and top quarks.},
Doi = {10.1140/epjc/s10052-020-8227-9},
Key = {fds365426}
}
@article{fds308313,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu,
A},
Title = {Higgs boson studies at the Tevatron},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.88.052014},
Abstract = {We combine searches by the CDF and D0 Collaborations for the
standard model Higgs boson with mass in the range 90-200
GeV/c2 produced in the gluon-gluon fusion, WH, ZH, tt̄H,
and vector boson fusion processes, and decaying in the
H→bb̄, H→W+W-, H→ZZ, H→τ+τ-, and H→γγ modes.
The data correspond to integrated luminosities of up to 10
fb-1 and were collected at the Fermilab Tevatron in pp̄
collisions at √s=1.96 TeV. The searches are also
interpreted in the context of fermiophobic and fourth
generation models. We observe a significant excess of events
in the mass range between 115 and 140 GeV/c2. The local
significance corresponds to 3.0 standard deviations at
mH=125 GeV/c2, consistent with the mass of the Higgs boson
observed at the LHC, and we expect a local significance of
1.9 standard deviations. We separately combine searches for
H→bb̄, H→W +W-, H→τ+τ-, and H→γγ. The observed
signal strengths in all channels are consistent with the
presence of a standard model Higgs boson with a mass of 125
GeV/c2. © 2013 American Physical Society.},
Doi = {10.1103/PhysRevD.88.052014},
Key = {fds308313}
}
@article{fds321299,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas,
AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus,
M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Bedikian, S and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger,
N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius,
C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black,
CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet,
D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli,
R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole,
B},
Title = {Identification and energy calibration of hadronically
decaying tau leptons with the ATLAS experiment in pp
collisions at [Formula: see text][Formula: see
text].},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {303},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3500-z},
Abstract = {This paper describes the trigger and offline reconstruction,
identification and energy calibration algorithms for
hadronic decays of tau leptons employed for the data
collected from <i>pp</i> collisions in 2012 with the ATLAS
detector at the LHC center-of-mass energy [Formula: see
text] [Formula: see text]. The performance of these
algorithms is measured in most cases with [Formula: see
text] decays to tau leptons using the full 2012 dataset,
corresponding to an integrated luminosity of 20.3
fb[Formula: see text]. An uncertainty on the offline
reconstructed tau energy scale of 2-4 %, depending on
transverse energy and pseudorapidity, is achieved using two
independent methods. The offline tau identification
efficiency is measured with a precision of 2.5 % for
hadronically decaying tau leptons with one associated track,
and of 4 % for the case of three associated tracks,
inclusive in pseudorapidity and for a visible transverse
energy greater than 20 [Formula: see text]. For hadronic tau
lepton decays selected by offline algorithms, the tau
trigger identification efficiency is measured with a
precision of 2-8 %, depending on the transverse energy. The
performance of the tau algorithms, both offline and at the
trigger level, is found to be stable with respect to the
number of concurrent proton-proton interactions and has
supported a variety of physics results using hadronically
decaying tau leptons at ATLAS.},
Doi = {10.1140/epjc/s10052-015-3500-z},
Key = {fds321299}
}
@article{fds321211,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister,
I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero,
J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman,
JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn,
AP},
Title = {Identification of boosted, hadronically decaying W
bosons and comparisons with ATLAS data taken at [Formula:
see text] TeV.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {154},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-3978-z},
Abstract = {This paper reports a detailed study of techniques for
identifying boosted, hadronically decaying <i>W</i> bosons
using 20.3 fb[Formula: see text] of proton-proton collision
data collected by the ATLAS detector at the LHC at a
centre-of-mass energy [Formula: see text]. A range of
techniques for optimising the signal jet mass resolution are
combined with various jet substructure variables. The
results of these studies in Monte Carlo simulations show
that a simple pairwise combination of groomed jet mass and
one substructure variable can provide a 50 % efficiency for
identifying <i>W</i> bosons with transverse momenta larger
than 200 GeV while maintaining multijet background
efficiencies of 2-4 % for jets with the same transverse
momentum. These signal and background efficiencies are
confirmed in data for a selection of tagging
techniques.},
Doi = {10.1140/epjc/s10052-016-3978-z},
Key = {fds321211}
}
@article{fds321198,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Identification of high transverse momentum top quarks in pp
collisions at √s= 8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {6},
Publisher = {Springer Nature},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2016)093},
Abstract = {This paper presents studies of the performance of several
jet-substructure techniques, which are used to identify
hadronically decaying top quarks with high transverse
momentum contained in large-radius jets. The efficiency of
identifying top quarks is measured using a sample of
top-quark pairs and the rate of wrongly identifying jets
from other quarks or gluons as top quarks is measured using
multijet events collected with the ATLAS experiment in 20.3
fb−1of 8 TeV proton-proton collisions at the Large Hadron
Collider. Predictions from Monte Carlo simulations are found
to provide an accurate description of the performance. The
techniques are compared in terms of signal efficiency and
background rejection using simulations, covering a larger
range in jet transverse momenta than accessible in the
dataset. Additionally, a novel technique is developed that
is optimized to reconstruct top quarks in events with many
jets.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP06(2016)093},
Key = {fds321198}
}
@article{fds308891,
Author = {al, FAE},
Title = {Identification of top quarks using kinematic
variables},
Journal = {Phys. Rev. D},
Volume = {52},
Number = {5},
Pages = {R2605-R2609},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.52.R2605},
Abstract = {We have used a kinematic technique to distinguish top quark
pair production from background in pp collisions at s=1.8
TeV, applied to 67 pb-1 of data. We define a sample of W+3
jet events in which the jets are produced at large angles
relative to the incident beams. In this sample, we find an
excess of events with large jet transverse energies relative
to expectations from background. The excess is consistent
with top quark production; a large fraction of events in
this kinematic region contains b jets. We interpret these
results as evidence that most of the selected events are
from tt decay.},
Doi = {10.1103/PhysRevD.52.R2605},
Key = {fds308891}
}
@article{fds308431,
Author = {Aaltonen, T and ÁlvarezGonzález, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan,
A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg,
C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd,
S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha,
C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen,
YC and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
ME and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De Cecco and S},
Title = {Improved determination of the sample composition of dimuon
events produced in pp̄ collisions at √s=1.96
TeV},
Journal = {European Physical Journal C},
Volume = {71},
Number = {8},
Pages = {1-14},
Publisher = {Springer Nature},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-011-1720-4},
Abstract = {We use a new method to estimate with 5% accuracy the
contribution of pion and kaon in-flight-decays to the dimuon
data set acquired with the CDF detector. Based on this
improved estimate, we show that the total number and the
properties of the collected dimuon events are not yet
accounted for by ordinary sources of dimuons which also
include the contributions, as measured in the data, of heavy
flavor, Υ{hooked}, and Drell-Yan production in addition to
muons mimicked by hadronic punchthrough. The number of
unaccounted events corresponds to (12.8±3.2)% of the bb̄
production. We find that (23±6)% of the unaccounted events
contain additional muon candidates. For comparison, this
fraction is (6.9±0.4)% for events due to bb̄ production.
© 2011 The Author(s).},
Doi = {10.1140/epjc/s10052-011-1720-4},
Key = {fds308431}
}
@article{fds308507,
Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco,
SD and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shekhar, R and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki, M and Denis,
RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini,
N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez,
F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang,
T},
Title = {Improved search for a Higgs boson produced in association
with Z→l+l- in pp̄ collisions at
√s=1.96TeV},
Journal = {Physical Review Letters},
Volume = {105},
Number = {25},
Pages = {251802},
Year = {2010},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.251802},
Abstract = {We search for the standard model Higgs boson produced with a
Z boson in 4.1fb⊃-1 of integrated luminosity collected
with the CDF II detector at the Tevatron. In events
consistent with the decay of the Higgs boson to a
bottom-quark pair and the Z boson to electrons or muons, we
set 95% credibility level upper limits on the ZH production
cross section multiplied by the H→bb̄ branching ratio.
Improved analysis methods enhance signal sensitivity by 20%
relative to previous searches. At a Higgs boson mass of
115GeV/c2 we set a limit of 5.9 times the standard model
cross section. © 2010 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.105.251802},
Key = {fds308507}
}
@article{fds308730,
Author = {al, DAE},
Title = {Inclusive Double-Pomeron Exchange at the Fermilab Tevatron
p-barp Collide},
Journal = {Physical Review Letters},
Volume = {93},
Number = {14},
Pages = {141601},
Year = {2004},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.93.141601},
Abstract = {We report results from a study of events with a double-
Pomeron exchange topology produced in p-barp collisions at
sqrt[s]=1800 GeV. The events are characterized by a leading
antiproton and a large rapidity gap on the outgoing proton
side. We find that the differential production cross section
agrees in shape with predictions based on Regge theory and
factorization, and that the ratio of double-Pomeron exchange
to single diffractive production rates is relatively
unsuppressed as compared to the O(10) suppression factor
previously measured in single diffractive
production.},
Doi = {10.1103/physrevlett.93.141601},
Key = {fds308730}
}
@article{fds308871,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Auchincloss, P and Azfar,
F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov,
S and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
S and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M},
Title = {Inclusive Jet Cross Section in p-barp Collisions at sqrt
s=1.8 TeV.},
Journal = {Physical review letters},
Volume = {77},
Number = {3},
Pages = {438-443},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.77.438},
Abstract = {The inclusive jet differential cross section has been
measured for jet transverse energies, ET, from 15 to 440
GeV, in the pseudorapidity region 0.1 [Formula preented].
The results are based on 19.5 pb−1 of data collected by
the CDF collaboration at the Fermilab Tevatron collider. The
data are compared with QCD predictions for various sets of
parton distribution functions. The cross section for jets
with ET > 200 GeV is significantly higher than current
predictions based on O(α3s) perturbative QCD calculations.
Various possible explanations for the high-ET excess are
discussed. © 1996 The American Physical
Society.},
Doi = {10.1103/physrevlett.77.438},
Key = {fds308871}
}
@article{fds308732,
Author = {al, DAE},
Title = {Inclusive Search for Anomalous Production of High-pT
Like-Sign Lepton Pairs in pp-bar Collisions at sqrt[s]=1.8
TeV},
Journal = {Physical Review Letters},
Volume = {93},
Number = {6},
Pages = {061802},
Year = {2004},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.93.061802},
Abstract = {We report on a search for anomalous production of events
with at least two charged, isolated, like-sign leptons, each
with pT>11 GeV/c using a 107 pb-1 sample of 1.8 TeV pp-bar
collisions collected by the CDF detector. We define a signal
region containing low background from standard model
processes. To avoid bias, we fix the final cuts before
examining the event yield in the signal region using control
regions to test the Monte Carlo predictions. We observe no
events in the signal region, consistent with an expectation
of 0.63+0.84-0.07 events. We present 95% confidence level
limits on new physics processes in both a signature-based
context as well as within a representative minimal
supergravity (tan( beta =3) model.},
Doi = {10.1103/physrevlett.93.061802},
Key = {fds308732}
}
@article{fds308627,
Author = {Abulencia, and A, and others},
Title = {Inclusive search for new physics with like-sign dilepton
events in $p \bar{p}$ collisions at $\sqrt{s}$ =
1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {22},
Pages = {221803},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.221803},
Abstract = {We describe a search for anomalous production of events with
two leptons (e or µ) of the same electric charge in
p[overline p] collisions at a center-of-mass energy of 1.96
TeV. Many extensions to the standard model predict the
production of two leptons of the same electric charge. This
search has a significant increase in sensitivity compared to
earlier searches. Using a data sample corresponding to 1
fb-1 of integrated luminosity recorded by the CDF II
detector, we observe no significant excess in an inclusive
selection (expect 33.2$\pm$4.7 events, observe 44) or in a
supersymmetry-optimized selection (expect 7.8$\pm$1.1
events, observe 13.)},
Doi = {10.1103/physrevlett.98.221803},
Key = {fds308627}
}
@article{fds308530,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher,
A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi,
C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and da Costa, JG and Gunay-Unalan, Z and Haber, C and Hahn,
K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher,
F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko,
BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal,
AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone,
S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Griso,
SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts,
K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder,
N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
A and Ramakrishnan, V and Ranjan, N and Redondo, I and Rekovic, V and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt,
MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider,
FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas,
J},
Title = {Inclusive search for squark and gluino production in pp[over
] collisions at sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {102},
Number = {12},
Pages = {121801},
Year = {2009},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.102.121801},
Abstract = {We report on a search for inclusive production of squarks
and gluinos in pp[over ] collisions at sqrt[s]=1.96 TeV, in
events with large missing transverse energy and multiple
jets of hadrons in the final state. The study uses a CDF Run
II data sample corresponding to 2 fb(-1) of integrated
luminosity. The data are in good agreement with the standard
model predictions, giving no evidence for any squark or
gluino component. In an R-parity conserving minimal
supergravity scenario with A(0)=0, mu<0, and tanbeta=5, 95%
C.L. upper limits on the production cross sections in the
range between 0.1 and 1 pb are obtained, depending on the
squark and gluino masses considered. For gluino masses below
280 GeV/c(2), arbitrarily large squark masses are excluded
at the 95% C.L., while for mass degenerate gluinos and
squarks, masses below 392 GeV/c(2) are excluded at the 95%
C.L.},
Doi = {10.1103/physrevlett.102.121801},
Key = {fds308530}
}
@article{fds308486,
Author = {Aaltonen, and T, and others},
Title = {Inclusive Search for Standard Model Higgs Boson Production
in the WW Decay Channel using the CDF II
Detector},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {6},
Pages = {061803},
Year = {2010},
url = {http://arXiv.org/abs/1001.4468},
Abstract = {http://arxiv.org/abs/1001.4468},
Doi = {10.1103/PhysRevLett.104.061803},
Key = {fds308486}
}
@article{fds308275,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Indirect measurement of sin2θW (or MW) using μ+μ- pairs
from γ* /Z bosons produced in p p ̄ collisions at a
center-of-momentum energy of 1.96 TeV INDIRECT MEASUREMENT
of sin2θW (OR ... T. AALTONEN et al.},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {7},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.89.072005},
Abstract = {Drell-Yan lepton pairs are produced in the process
pp̄→μ+μ- +X through an intermediate γ*/Zboson. The
forward-backward asymmetry in the polar-angle distribution
of the μ- as a function of the invariant mass of the μ+μ-
pair is used to obtain the effective leptonic determination
sin2θefflept of the electroweak-mixing parameter sin2θW,
from which the value of sin2θW is derived assuming the
standard model. The measurement sample, recorded by the
Collider Detector at Fermilab (CDF), corresponds to 9.2fb-1
of integrated luminosity from pp̄ collisions at a
center-of-momentum energy of 1.96 TeV, and is the full CDF
Run II data set. The value of sin2θefflept is found to be
0.2315±0. 0010, where statistical and systematic
uncertainties are combined in quadrature. When interpreted
within the context of the standard model using the on-shell
renormalization scheme, where sin2θW=1-MW2/MZ2, the
measurement yields sin2θW=0.2233±0.0009, or equivalently a
W-boson mass of 80.365±0.047GeV/c2. The value of the
W-boson mass is in agreement with previous determinations in
electron-positron collisions and at the Tevatron collider.
© 2014 American Physical Society.},
Doi = {10.1103/PhysRevD.89.072005},
Key = {fds308275}
}
@article{fds308306,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Indirect measurement of sin2θw (MW)
using e+e- pairs in the Z-boson region
with p̄p collisions at a center-of-momentum energy of 1.96
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.88.072002},
Abstract = {Drell-Yan lepton pairs are produced in the process p̄p→e
+e-+X through an intermediate γ*/Z boson. The lepton
angular distributions are used to provide information on the
electroweak-mixing parameter sin2θw via its observable
effective-leptonic sin2θw, or sinâ¡2θefflept. A new
method to infer sin 2θw or, equivalently, the W-boson mass
MW in the on-shell scheme, is developed and tested using a
previous CDF Run II measurement of angular distributions
from electron pairs in a sample corresponding to 2.1 fb-1 of
integrated luminosity from p̄p collisions at a
center-of-momentum energy of 1.96 TeV. The value of
sinâ¡2θefflept is found to be 0.2328±0.0011. Within a
specified context of the standard model, this results in sin
2θw=0.2246±0.0011, which corresponds to a W-boson mass of
80.297±0.055 GeV/c2, in agreement with previous
determinations in electron-position collisions and at the
Tevatron collider. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.072002},
Key = {fds308306}
}
@article{fds375901,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Castillo, FL and Costanza, F and Delmastro, M and Di
Ciaccio, L and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo
Martinez, N and Poddar, G and Sanchez Pineda and A and Sauvan, E and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Li, T and Marchiori, G and Nakkalil, K and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wamorkar, T and Wang, R and Zhang, J and Cheu, E and Cui, Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost,
M},
Title = {Integrated and differential fiducial cross-section
measurements for the vector boson fusion production of the
Higgs boson in the H →WW∗→eνμν decay channel at 13
TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {108},
Number = {7},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.108.072003},
Abstract = {The vector-boson production cross section for the Higgs
boson decay in the Formula Presented channel is measured as
a function of kinematic observables sensitive to the Higgs
boson production and decay properties as well as integrated
in a fiducial phase space. The analysis is performed using
the proton-proton collision data collected by the ATLAS
detector in Run 2 of the LHC at Formula Presented
center-of-mass energy, corresponding to an integrated
luminosity of Formula Presented. The different flavor final
state is studied by selecting an electron and a muon
originating from a pair of Formula Presented bosons and
compatible with the Higgs boson decay. The data are
corrected for the effects of detector inefficiency and
resolution, and the measurements are compared with different
state-of-the-art theoretical predictions. The differential
cross sections are used to constrain anomalous interactions
described by dimension-six operators in an effective field
theory.},
Doi = {10.1103/PhysRevD.108.072003},
Key = {fds375901}
}
@article{fds308791,
Author = {Affolder, A and Azzi-Bacchetta, P and Bacchetta, N and Barker, G and Barbaro-Galtieri, A and Basti, A and Bedeschi, F and Bisello, D and Blusk, S and Caskey, WP and Chiarelli, G and Connolly, A and Demina, R and Ely, R and Field, R and Garcia-Sciveres, M and Giolo, K and Goldstein,
D and Goldstein, J and Grim, GP and Guerzoni, M and Haas, R and Haber, C and Hara, K and Hartmann, F and Heiss, A and Hill, C and Hrycyk, M and Incandela, J and Kato, Y and Knoblauch, D and Kruse, M and Lander, RL and Lei, CM and Leonardi, GL and Leone, S and Miyazaki, Y and Moggi, A and Muller, T and Munar-Ara, A and Okusawa, T and Palmonari, F and Paulini,
M and Piacentino, G and Pellett, DE and Raffaelli, F and Roederer, F and Saltzberg, D and Shimojima, M and Stuart, D and Suzuki, H and Takano, T and Takikawa, K and Tanaka, M and Taniguchi, Y and Tipton, P and Turini, N and Volobouev, I and Wenzel, H and Wilkes, TD and Yao, W and Yoshida, T and Zetti, F and Zucchelli, S},
Title = {Intermediate Silicon Layers detector for the CDF
experiment},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {453},
Number = {1-2},
Pages = {84-88},
Publisher = {Elsevier BV},
Year = {2000},
Month = {October},
url = {http://dx.doi.org/10.1016/S0168-9002(00)00610-0},
Abstract = {The Intermediate Silicon Layers (ISL) detector is currently
being built as part of the CDF II detector upgrade project.
The ISL detector will significantly improve tracking in the
central region and, together with the Silicon Vertex
detector, provide stand-alone 3D track information in the
forward/backward regions. In this article, we present the
quality of the production sensors manufactured by Hamamatsu
Photonics, which account for roughly half of the silicon
sensors used in the ISL detector.},
Doi = {10.1016/S0168-9002(00)00610-0},
Key = {fds308791}
}
@article{fds308439,
Author = {Aaltonen, and T, and al, E},
Title = {Invariant Mass Distribution of Jet Pairs Produced in
Association with a ${W}$ Boson in $p\overline{p}$ Collisions
at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {17},
Pages = {171801},
Publisher = {American Physical Society},
Year = {2011},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.171801},
Abstract = {We report a study of the invariant mass distribution of jet
pairs produced in association with a W boson using data
collected with the CDF detector which correspond to an
integrated luminosity of 4.3 fb(-1). The observed
distribution has an excess in the 120-160 GeV/c(2) mass
range which is not described by current theoretical
predictions within the statistical and systematic
uncertainties. In this Letter, we report studies of the
properties of this excess.},
Doi = {10.1103/PhysRevLett.106.171801},
Key = {fds308439}
}
@article{fds308271,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Invariant-mass distribution of jet pairs produced in
association with a W boson in p p ̄ collisions at s
=1.96TeV using the full CDF Run II data set invariant-mass
distribution of ⋯ T. Aaltonen et al.},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {9},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.89.092001},
Abstract = {We report on a study of the dijet invariant-mass
distribution in events with one identified lepton, a
significant imbalance in the total event transverse
momentum, and two jets. This distribution is sensitive to
the possible production of a new particle in association
with a W boson, where the boson decays leptonically. We use
the full data set of proton-antiproton collisions at 1.96
TeV center-of-mass energy collected by the Collider Detector
at the Fermilab Tevatron, corresponding to an integrated
luminosity of 8.9fb-1. The data are found to be consistent
with standard model expectations, and a 95% confidence level
upper limit is set on the production cross section of a W
boson in association with a new particle decaying into two
jets. © 2014 American Physical Society.},
Doi = {10.1103/PhysRevD.89.092001},
Key = {fds308271}
}
@article{fds308869,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and De-Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas,
A and Berge, JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner,
N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cronin-Hennessy, D and Culbertson,
R and Daniels, T and De Jongh and F and Delchamps, S and Dell’agnello, S and Dell’orso, M and Demina, R and Demortier, L},
Title = {J/ψ and ψ(2s) Production pp collisions at √ s =
1.8TeV},
Journal = {Physical Review Letters},
Volume = {79},
Number = {4},
Pages = {572-577},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.572},
Abstract = {We present a study of J/ψ and ψ(2S) production in pp
collisons at √ s = 1.8 TeV with the CDF detector at
Fermilab. The J/ψ and ψ(2S) mesons are reconstructed using
their μ+μ− decay modes. We have measured the inclusive
production cross section for both mesons as a function of
their transverse momentum in the central region, η < 0.6.
We also measure the fraction of these events originating
from b hadrons. We thus extract individual cross sections
for J/ψ and ψ 2(S) mesons from b-quark decays and prompt
production. We find a large excess (approximately a factor
of 50) of direct ψ(2S) production compared with predictions
from the color singlet model. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.79.572},
Key = {fds308869}
}
@article{fds321273,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes,
GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burghgrave,
B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey,
P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH},
Title = {Jet energy measurement and its systematic uncertainty in
proton-proton collisions at [Formula: see text] TeV with
the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Pages = {17},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3190-y},
Abstract = {The jet energy scale (JES) and its systematic uncertainty
are determined for jets measured with the ATLAS detector
using proton-proton collision data with a centre-of-mass
energy of [Formula: see text] TeV corresponding to an
integrated luminosity of [Formula: see text][Formula: see
text]. Jets are reconstructed from energy deposits forming
topological clusters of calorimeter cells using the
anti-[Formula: see text] algorithm with distance parameters
[Formula: see text] or [Formula: see text], and are
calibrated using MC simulations. A residual JES correction
is applied to account for differences between data and MC
simulations. This correction and its systematic uncertainty
are estimated using a combination of in situ techniques
exploiting the transverse momentum balance between a jet and
a reference object such as a photon or a [Formula: see text]
boson, for [Formula: see text] and pseudorapidities
[Formula: see text]. The effect of multiple proton-proton
interactions is corrected for, and an uncertainty is
evaluated using in situ techniques. The smallest JES
uncertainty of less than 1 % is found in the central
calorimeter region ([Formula: see text]) for jets with
[Formula: see text]. For central jets at lower [Formula: see
text], the uncertainty is about 3 %. A consistent JES
estimate is found using measurements of the calorimeter
response of single hadrons in proton-proton collisions and
test-beam data, which also provide the estimate for
[Formula: see text] TeV. The calibration of forward jets is
derived from dijet [Formula: see text] balance measurements.
The resulting uncertainty reaches its largest value of 6 %
for low-[Formula: see text] jets at [Formula: see text].
Additional JES uncertainties due to specific event
topologies, such as close-by jets or selections of event
samples with an enhanced content of jets originating from
light quarks or gluons, are also discussed. The magnitude of
these uncertainties depends on the event sample used in a
given physics analysis, but typically amounts to
0.5-3 %.},
Doi = {10.1140/epjc/s10052-014-3190-y},
Key = {fds321273}
}
@article{fds365380,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Jet energy scale and resolution measured in proton–proton
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {8},
Year = {2021},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09402-3},
Abstract = {Jet energy scale and resolution measurements with their
associated uncertainties are reported for jets using
36–81 fb- 1 of proton–proton collision data with a
centre-of-mass energy of s=13 TeV collected by the ATLAS
detector at the LHC. Jets are reconstructed using two
different input types: topo-clusters formed from energy
deposits in calorimeter cells, as well as an algorithmic
combination of charged-particle tracks with those
topo-clusters, referred to as the ATLAS particle-flow
reconstruction method. The anti-kt jet algorithm with radius
parameter R= 0.4 is the primary jet definition used for both
jet types. This result presents new jet energy scale and
resolution measurements in the high pile-up conditions of
late LHC Run 2 as well as a full calibration of
particle-flow jets in ATLAS. Jets are initially calibrated
using a sequence of simulation-based corrections. Next,
several in situ techniques are employed to correct for
differences between data and simulation and to measure the
resolution of jets. The systematic uncertainties in the jet
energy scale for central jets (| η| < 1.2) vary from 1% for
a wide range of high-pT jets (250<pT<2000GeV), to 5% at very
low pT (20GeV) and 3.5% at very high pT (>2.5TeV). The
relative jet energy resolution is measured and ranges from
(24 ± 1.5)% at 20 GeV to (6 ± 0.5)% at
300 GeV.},
Doi = {10.1140/epjc/s10052-021-09402-3},
Key = {fds365380}
}
@article{fds308902,
Author = {al, FAE},
Title = {Kinematic evidence for top-quark pair production in w plus
multijet events in p(p)over-bar collisions at root-s=1.8
tev},
Journal = {Phys. Rev. D},
Volume = {51},
Number = {9},
Pages = {4623-4637},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevd.51.4623},
Abstract = {© 1995 The American Physical Society We present a study of
W+multijet events that compares the kinematics of the
observed events with expectations from direct QCD W+jet
production and from production and decay of top quark pairs.
The data were collected in the 1992-93 run with the Collider
Detector at Fermilab (CDF) from 19.3 pb-1 of
proton-antiproton collisions at s =1.8 TeV. A W+2 jet sample
and a W+3 jet sample are selected with the requirement that
at least the two or three jets have energy transverse with
respect to the beam axis in excess of 20 GeV. The jet energy
distributions for the W+2 jet sample agree well with the
predictions of direct QCD W production. From the W+3 jet
events, a "signal sample" with an improved ratio of tt̄ to
QCD produced W events is selected by requiring each jet to
be emitted centrally in the event center of mass frame. This
sample contains 14 events with unusually hard jet ET
distributions not well described by expectations for jets
from direct QCD W production and other background processes.
Using expected jet ET distributions, a relative likelihood
is defined and used to determine if an event is more
consistent with the decay of tt̄ pairs, with Mtop=170
GeV/c2, than with direct QCD W production. Eight of the 14
signal sample events are found to be more consistent with
top-quark than direct QCD W production, while only 1.7 such
top-quark-like events are expected in the absence of tt̄.
The probability that the observation is due to an upward
fluctuation of the number of background events is found to
be 0.8%. The robustness of the result was tested by varying
the cuts defining the signal sample, and the largest
probability for such a fluctuation found was 1.9%. Good
agreement in the jet spectra is obtained if jet production
from tt̄ pair decays is included. For those events
kinematically more consistent with tt̄ we find evidence for
a b-quark content in their jets to the extent expected from
top quark decay, and larger than expected for background
processes. For events with four or more jets, the
discrepancy with the predicted jet distributions from direct
QCD W production, and the associated excess of b-quark
content, is more pronounced.},
Doi = {10.1103/physrevd.51.4623},
Key = {fds308902}
}
@article{fds340919,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbara, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bikhari, W and Bolla,
G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Burner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir,
S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch,
H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel,
O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti,
G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn,
SR and Hamilton, R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hausser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman,
KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman,
BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins,
D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch,
L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo,
K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald,
W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone,
S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson,
C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Volobouev, I and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund,
AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu,
X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Kinematics of tt̄ events at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {59},
Number = {9},
Pages = {1-20},
Year = {1999},
url = {http://dx.doi.org/10.1103/PhysRevD.59.092001},
Abstract = {The kinematic properties of tt̄ events are studied in the
W+ multijet channel using data collected with the CDF
detector during the 1992-1995 runs at the Fermilab Tevatron
collider corresponding to an integrated luminosity of 109
pb-1. Distributions of a variety of kinematic variables
chosen to be sensitive to different aspects of tt̄
production are compared with those expected from Monte Carlo
calculations. A sample of 34 events rich in tt̄ pairs is
obtained by requiring at least one jet identified by the
silicon vertex detector (SVX) as having a displaced vertex
consistent with the decay of a b hadron. The data are found
to be in good agreement with predictions of the leading
order tt̄ matrix element with color coherent parton shower
evolution. ©1999 The American Physical Society.},
Doi = {10.1103/PhysRevD.59.092001},
Key = {fds340919}
}
@article{fds308726,
Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
J and Culbertson, R and Dagenhart, D and D'Auria, S and De Barbaro and P and Cecco, SD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi,
C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede,
S},
Title = {KS0 and Λ0 production studies in pp̄ collisions at s=1800
and 630 GeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {72},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.72.052001},
Abstract = {We present a study of the production of KS0 and Λ0 in
inelastic pp̄ collisions at s=1800 and 630 GeV using data
collected by the CDF experiment at the Fermilab Tevatron.
Analyses of KS0 and Λ0 multiplicity and transverse momentum
distributions, as well as of the dependencies of the average
number and pT of KS0 and Λ0 on charged particle
multiplicity, are reported. Systematic comparisons are
performed for the full sample of inelastic collisions, and
for the low and high momentum transfer subsamples, at the
two energies. The pT distributions extend above 8GeV/c,
showing a pT higher than previous measurements. The
dependence of the mean KS0(Λ0) pT on the charged particle
multiplicity for the three samples shows a behavior
analogous to that of charged primary tracks. © 2005 The
American Physical Society.},
Doi = {10.1103/PhysRevD.72.052001},
Key = {fds308726}
}
@article{fds321360,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau,
M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli,
F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura,
AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
M},
Title = {Light-quark and gluon jet discrimination in [Formula: see
text] collisions at [Formula: see text] with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {8},
Pages = {3023},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3023-z},
Abstract = {A likelihood-based discriminant for the identification of
quark- and gluon-initiated jets is built and validated using
4.7 fb[Formula: see text] of proton-proton collision data
at [Formula: see text] [Formula: see text] collected with
the ATLAS detector at the LHC. Data samples with enriched
quark or gluon content are used in the construction and
validation of templates of jet properties that are the input
to the likelihood-based discriminant. The discriminating
power of the jet tagger is established in both data and
Monte Carlo samples within a systematic uncertainty of
[Formula: see text] 10-20 %. In data, light-quark jets can
be tagged with an efficiency of [Formula: see text] while
achieving a gluon-jet mis-tag rate of [Formula: see text] in
a [Formula: see text] range between [Formula: see text] and
[Formula: see text] for jets in the acceptance of the
tracker. The rejection of gluon-jets found in the data is
significantly below what is attainable using a Pythia 6
Monte Carlo simulation, where gluon-jet mis-tag rates of
10 % can be reached for a 50 % selection efficiency of
light-quark jets using the same jet properties.},
Doi = {10.1140/epjc/s10052-014-3023-z},
Key = {fds321360}
}
@article{fds308433,
Author = {Aaltonen, and T, and al, E},
Title = {Limits on Anomalous Trilinear Gauge Couplings in ${Z}\gamma$
Events from $p\overline{p}$ Collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {5},
Pages = {051802},
Publisher = {American Physical Society},
Year = {2011},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.051802},
Abstract = {Using Zγ candidate events collected by the CDF detector at
the Tevatron Collider, we search for potential anomalous
(non-standard-model) couplings between the Z boson and the
photon. Zγ couplings vanish at tree level and are heavily
suppressed at higher orders; hence any evidence of couplings
indicates new physics. Measurements are performed using data
corresponding to an integrated luminosity of 4.9 fb(-1)
in the Z→νν¯ decay channel and 5.1 fb(-1) in the
Z→l(+)l(-) (l=μ, e) decay channels. The combination of
these measurements provides the most stringent limits to
date on Zγ trilinear gauge couplings. Using an energy scale
of Λ=1.5 TeV to allow for a direct comparison with
previous measurements, we find limits on the CP-conserving
parameters that describe Zγ couplings to be
|h(3)(γ,Z)|<0.022 and |h(4)(γ,Z)|<0.0009. These results
are consistent with standard model predictions.},
Doi = {10.1103/PhysRevLett.107.051802},
Key = {fds308433}
}
@article{fds308635,
Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Behari,
S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak,
M},
Title = {Limits on anomalous triple gauge couplings in pp̄
collisions at s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {76},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2007},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.76.111103},
Abstract = {We present a search for anomalous triple gauge couplings
(ATGC) in WW and WZ boson production. The boson pairs are
produced in pp̄ collisions at s=1.96TeV, and the data
sample corresponds to 350pb-1 of integrated luminosity
collected with the CDF II detector at the Fermilab Tevatron.
In this search one W decays to leptons, and the other boson
(W or Z) decays hadronically. Combining with a previously
published CDF measurement of Wγ boson production yields
ATGC limits of -0.18<λ<0.17 and -0.46<Δκ<0.39 at the 95%
confidence level, using a cutoff scale Λ=1.5TeV. © 2007
The American Physical Society.},
Doi = {10.1103/PhysRevD.76.111103},
Key = {fds308635}
}
@article{fds308756,
Author = {al, DAE},
Title = {Limits on Extra Dimensions and New Particle Production in
the Exclusive Photon and Missing Energy Signature in pp-bar
Collisions at sqrt[s]=1.8 TeV},
Journal = {Physical Review Letters},
Volume = {89},
Number = {28 Pt 1},
Pages = {281801},
Year = {2002},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.89.281801},
Abstract = {The exclusive gamma E̸T signal has a small standard
model cross section and is thus a channel sensitive to new
physics. This signature is predicted by models with a
superlight gravitino or with large extra spatial dimensions.
We search for such signals at the Collider Detector at
Fermilab, using 87 pb-1 of data at sqrt[s]=1.8 TeV, and
extract 95% C.L. limits on these processes. A limit of
221 GeV is set on the scale |F|1/2 in supersymmetric
models. For 4, 6, and 8 extra dimensions, model- dependent
limits on the fundamental mass scale MD of 0.55, 0.58, and
0.60 TeV, respectively, are found. We also specify a
"pseudo-model- independent" method of comparing the results
to theoretical predictions.},
Doi = {10.1103/physrevlett.89.281801},
Key = {fds308756}
}
@article{fds308856,
Author = {al, FAE},
Title = {Limits on quark-lepton compositeness scales from dileptons
produced in 1.8 TeV p(p)over-bar collisions},
Journal = {Phys. Rev. Lett.},
Volume = {79},
Number = {12},
Pages = {2198-2203},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.2198},
Abstract = {The dilepton mass spectrum in pp-→|+|-+X interactions is
studied using dielectrons (ee) and dimuons (μμ) in 100 pb-
of data collected with the Collider Detector at Fermilab.
The data are consistent with standard model predictions. The
mass spectrum, being a probe for new physics, is examined
for new interactions of quarks and leptons from a common
composite structure. Assuming a contact interaction with the
conventional coupling g20/4π = 1, limits on chiral
quark-electron and quark-muon compositeness scales in the
range of 2.5 to 4.2 TeV are obtained. © 1997 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.79.2198},
Key = {fds308856}
}
@article{fds308894,
Author = {al, FAE},
Title = {Limits on wwz and ww-gamma couplings from ww and wz
production in p(p)over-bar collisions at root-s=1.8
tev},
Journal = {Phys. Rev. Lett.},
Volume = {75},
Number = {6},
Pages = {1017-1022},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevLett.75.1017},
Abstract = {Direct limits are set on WWZ and WW three-boson couplings in
a search for WW and WZ production with high transverse
momentum in pp» collisions at s=1.8 TeV, using the Collider
Detector at Fermilab. The results are in agreement with the
SU(2) × U(1) model of electroweak interactions. Assuming
standard model WW couplings, the limits are interpreted as
direct evidence for a nonzero WWZ coupling at subprocess
energies near 500 GeV. Alternatively, assuming identical WWZ
and WW couplings, bounds -0.11< <2.27 and -0.81< <0.84 are
obtained at 95% C.L. for a form factor scale 1000 GeV. ©
1995 The American Physical Society.},
Doi = {10.1103/PhysRevLett.75.1017},
Key = {fds308894}
}
@article{fds308903,
Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman,
J},
Title = {Limits on Z-photon couplings from p-p-bar interactions at
sqrt s=1.8TeV.},
Journal = {Physical review letters},
Volume = {74},
Number = {11},
Pages = {1941-1945},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.74.1941},
Abstract = {We report limits on anomalous ZZ and Z couplings derived
from an analysis of Z+photon production based upon
approximately 20 pb-1 of the pp collision data recorded by
the Collider Detector at Fermilab. We observe good agreement
with the standard model expectation that all Z couplings are
zero. Confidence level intervals for individual couplings
and contours for pairs of CP-conserving/violating ZZ and Z
couplings are presented. © 1995 The American Physical
Society.},
Doi = {10.1103/physrevlett.74.1941},
Key = {fds308903}
}
@article{fds321145,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Luminosity determination in pp collisions at [Formula: see
text] = 8 TeV using the ATLAS detector at the
LHC.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {12},
Pages = {653},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4466-1},
Abstract = {The luminosity determination for the ATLAS detector at the
LHC during pp collisions at [Formula: see text] 8 TeV in
2012 is presented. The evaluation of the luminosity scale is
performed using several luminometers, and comparisons
between these luminosity detectors are made to assess the
accuracy, consistency and long-term stability of the
results. A luminosity uncertainty of [Formula: see text] is
obtained for the [Formula: see text] of pp collision data
delivered to ATLAS at [Formula: see text] 8 TeV in
2012.},
Doi = {10.1140/epjc/s10052-016-4466-1},
Key = {fds321145}
}
@article{fds375900,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Dos Santos and SPA and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH},
Title = {Luminosity determination in pp collisions at √s=13 TeV
using the ATLAS detector at the LHC},
Journal = {European Physical Journal C},
Volume = {83},
Number = {10},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11747-w},
Abstract = {The luminosity determination for the ATLAS detector at the
LHC during Run 2 is presented, with pp collisions at a
centre-of-mass energy s=13 TeV. The absolute luminosity
scale is determined using van der Meer beam separation scans
during dedicated running periods in each year, and
extrapolated to the physics data-taking regime using
complementary measurements from several luminosity-sensitive
detectors. The total uncertainties in the integrated
luminosity for each individual year of data-taking range
from 0.9% to 1.1%, and are partially correlated between
years. After standard data-quality selections, the full
Run 2 pp data sample corresponds to an integrated
luminosity of 140.1 ± 1.2 fb - 1 , i.e. an uncertainty of
0.83%. A dedicated sample of low-pileup data recorded in
2017–2018 for precision Standard Model physics
measurements is analysed separately, and has an integrated
luminosity of 338.1 ± 3.1 pb - 1 .},
Doi = {10.1140/epjc/s10052-023-11747-w},
Key = {fds375900}
}
@article{fds308274,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Mass and lifetime measurements of bottom and charm baryons
in p p ̄ collisions at s =1.96TeV MASS and LIFETIME
MEASUREMENTS of BOTTOM and ⋯ T. AALTONEN},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {April},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.89.072014},
Abstract = {We report on mass and lifetime measurements of several
ground state charmed and bottom baryons, using a data sample
corresponding to 9.6fb-1 from pp̄ collisions at s=1.96TeV
and recorded with the Collider Detector at Fermilab. Baryon
candidates are reconstructed from data collected with an
online event selection designed for the collection of
long-lifetime heavy-flavor decay products and a second event
selection designed to collect J/ ψ→μ+μ- candidates.
First evidence for the process Ωb-→Ωc0π- is presented
with a significance of 3.3σ. We measure the following
baryon masses: M(Ξc0)=2470.85±0.24(stat)
±0.55(syst)MeV/c2,M(Ξc+)=2468.00±0.18(stat)±0.51(syst)
MeV/c2,M(Λb)=5620.15±0.31(stat)±0.47(syst)MeV/c2,M(Ξb-)=
5793.4±1.8(stat)±0.7(syst)MeV/c2,M(Ξb0)=5788.7±4.3(stat)
±1.4(syst)MeV/c2,andM(Ωb-)=6047.5±3.8(stat)±0.6(syst)
MeV/c2.The isospin splitting of the Ξb-,0 states is found
to be M(Ξb-)-M(Ξb0)=4.7±4.7(stat)±0.7(syst)MeV/c2. The
isospin splitting of the Ξc0,+ states is found to be
M(Ξc0)-M(Ξc+)=2. 85±0.30(stat)±0.04(syst)MeV/c2. The
following lifetime measurements are made:
τ(Λb)=1.565±0.035(stat)±0. 020(syst)ps,τ(Ξb-)=1.32±0.14(stat)±0.02(syst)ps,
τ(Ωb-)=1.66-0.40+0.53(stat)±0.02(syst)ps. © 2014
American Physical Society.},
Doi = {10.1103/PhysRevD.89.072014},
Key = {fds308274}
}
@article{fds308665,
Author = {Acosta, and D, and others},
Title = {Measurement of $b$ hadron masses in exclusive $J/\psi$
decays with the CDF detector},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {20},
Pages = {202001},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.202001},
Abstract = {We measure the masses of $b$ hadrons in exclusively
reconstructed final states containing a $J/\psi\to\mu^-\mu^+$
decay using $\rm 220 pb^{-1}$ of data collected by the CDF
II experiment. We find: m(B^+) = 5279.10 \pm 0.41_{(stat.)}
\pm 0.36_{(sys.)} MeVcc, m(B^0) = 5279.63 \pm 0.53_{(stat.)}
\pm 0.33_{(sys.)} MeVcc, m(B^0_s) = 5366.01 \pm
0.73_{(stat.)} \pm 0.33_{(sys.)} MeVcc, m(\Lambda^0_b) =
5619.7 \pm 1.2_{(stat.)} \pm 1.2_{(sys.)} MeVcc. m(B^+) -
m(B^0) = -0.53 \pm 0.67_{(stat.)} \pm 0.14_{(sys.)} MeVcc,
m(B^0_s) - m(B^0) = 86.38 \pm 0.90_{(stat.)} \pm
0.06_{(sys.)} MeVcc m(\Lambda^0_b) - m(B^0) = 339.2 \pm
1.4_{(stat.)} \pm 0.1_{(sys.)} MeVcc. The measurements of
the $B^0_s$, $\Lambda^0_b$ mass, $m(B^0_s)-m(B^0)$ and
$m(\Lambda^0_b)-m(B^0)$ mass difference are of better
precision than the current world averages.},
Doi = {10.1103/physrevlett.96.202001},
Key = {fds308665}
}
@article{fds308453,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of $t\overline{t}$ spin correlation in
$p\overline{p}$ collisions using the CDF II detector at the
Tevatron},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {3},
Pages = {031104},
Publisher = {American Physical Society},
Year = {2011},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.83.031104},
Abstract = {The tt̄ spin correlation at production is a fundamental
prediction of QCD and a potentially incisive test of new
physics coupled to top quarks. We measure the tt̄ spin
state in pp̄ collisions at √s=1.96TeV using 1001
candidate events in the lepton plus jets decay channel
reconstructed in the CDF II detector. In the helicity basis,
for a top-quark mass of 172.5GeV/c2, we find a spin
correlation coefficient κ=0.60±0.50(stat)±0. 16(syst),
consistent with the QCD prediction, κ 0.40. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.83.031104},
Key = {fds308453}
}
@article{fds308494,
Author = {Aaltonen, and T, and others},
Title = {Measurement of $Z\gamma{}$ production in $pp[over
\ifmmode\bar\else\textasciimacron\fi{}]$ collisions at
$\sqrt{s}=1.96\,\,TeV$},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {3},
Pages = {031103},
Publisher = {American Physical Society},
Year = {2010},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.82.031103},
Abstract = {The production rate and kinematics of photons produced in
association with Z bosons are studied using 2fb-1 of pp̄
collision data collected at the Collider Detector at
Fermilab. The cross section for pp̄→"+-γ+X (where the
leptons " are either muons or electrons with dilepton mass
M>40GeV/c2, and where the photon has transverse energy
ETγ>7GeV and is well separated from the leptons) is
4.6±0.2(stat)±0.3(syst)±0.3(lum)pb, which is consistent
with standard model expectations. We use the photon ET
distribution from Zγ events where the Z has decayed to
μ+μ -, e+e-, or νν̄ to set limits on anomalous (non
standard model) trilinear couplings between photons and Z
bosons. © 2010 The American Physical Society.},
Doi = {10.1103/PhysRevD.82.031103},
Key = {fds308494}
}
@article{fds308443,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of ${b}$ Hadron Lifetimes in Exclusive Decays
Containing a ${J}/\psi$ in $p\overline{p}$ Collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {12},
Pages = {121804},
Publisher = {American Physical Society},
Year = {2011},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.121804},
Abstract = {We report on a measurement of b-hadron lifetimes in the
fully reconstructed decay modes B(+)→J/ψK(+),
B⁰→J/ψK*(892)⁰, B⁰→J/ψK(s)⁰, and
Λ(b)⁰→J/ψΛ⁰ using data corresponding to an
integrated luminosity of 4.3 fb⁻¹, collected by the CDF
II detector at the Fermilab Tevatron. The measured lifetimes
are τ(B(+))=[1.639±0.009(stat)±0.009(syst)] ps,
τ(B⁰)=[1.507±0.010(stat)±0.008(syst)] ps, and
τ(Λ(b)⁰)=[1.537±0.045(stat)±0.014(syst)] ps. The
lifetime ratios are τ(B(+))/τ(B⁰)=[1.088±0.009(stat)±0.004(syst)]
and τ(Λ(b)⁰)/τ(B⁰)=[1.020±0.030(stat)±0.008(syst)].
These are the most precise determinations of these
quantities from a single experiment.},
Doi = {10.1103/PhysRevLett.106.121804},
Key = {fds308443}
}
@article{fds308334,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach,
B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli,
F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behar Harpaz and S and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brown, G and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C},
Title = {Measurement of kT splitting scales in
W→ℓν events at [Formula: see text] with
the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {5},
Pages = {2432},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2432-8},
Abstract = {A measurement of splitting scales, as defined by the
<i>k</i><sub>T</sub> clustering algorithm, is presented for
final states containing a <i>W</i> boson produced in
proton-proton collisions at a centre-of-mass energy of
7 TeV. The measurement is based on the full 2010 data
sample corresponding to an integrated luminosity of
36 pb<sup>-1</sup> which was collected using the ATLAS
detector at the CERN Large Hadron Collider. Cluster
splitting scales are measured in events containing <i>W</i>
bosons decaying to electrons or muons. The measurement
comprises the four hardest splitting scales in a
<i>k</i><sub>T</sub> cluster sequence of the hadronic
activity accompanying the <i>W</i> boson, and ratios of
these splitting scales. Backgrounds such as multi-jet and
top-quark-pair production are subtracted and the results are
corrected for detector effects. Predictions from various
Monte Carlo event generators at particle level are compared
to the data. Overall, reasonable agreement is found with all
generators, but larger deviations between the predictions
and the data are evident in the soft regions of the
splitting scales.},
Doi = {10.1140/epjc/s10052-013-2432-8},
Key = {fds308334}
}
@article{fds308816,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari,
C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Breccia, L and Bromberg,
C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell,
M and Caner, A and Carithers, W and Carlsmith, D and Cassada, J and Castro,
A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Cropp, R and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui,
Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton,
R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi,
T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone,
S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson,
C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Portos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas,
J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidai, R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund,
AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu,
X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of b quark fragmentation fractions in the
production of strange and light B mesons in pp̄ collisions
at √s=1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {60},
Number = {9},
Pages = {1-14},
Year = {1999},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.60.092005},
Abstract = {A new technique to measure the ratio of b quark
fragmentation fractions in pp̄ collisions is described.
Using a 70-pb-1 sample of low-mass dimuon trigger data
recorded with the Collider Detector at Fermilab, we identify
B mesons by observing the double semileptonic decays b→c
μX with c→s μX. By counting the numbers of K*(892)0,
K*(892)+, and φ(1020) mesons produced in association with
these muon pairs, we measure the ratio of strange to
nonstrange B meson production to be fs/(fu+fd)=[21.0±3.6(stat)
-3.0+3.8(syst)]%. This measurement is the most precise
available from hadron collisions to date. Limits on the
branching fractions of semileptonic charm meson decays with
K1(1270), K1* (1410), and K2*(1430) mesons in the final
state are also obtained. ©1999 The American Physical
Society.},
Doi = {10.1103/PhysRevD.60.092005},
Key = {fds308816}
}
@article{fds314168,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and (CDF
Collaboration)},
Title = {Measurement of B(t→Wb)/B(t→Wq) in top-quark-pair decays
using dilepton events and the full CDF Run II data
set.},
Journal = {Physical review letters},
Volume = {112},
Number = {22},
Pages = {221801},
Year = {2014},
Month = {June},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.112.221801},
Abstract = {We present a measurement of the ratio of the top-quark
branching fractions R=B(t→Wb)/B(t→Wq), where q
represents any quark flavor, in events with two charged
leptons, imbalance in total transverse energy, and at least
two jets. The measurement uses proton-antiproton collision
data at center-of-mass energy 1.96 TeV, corresponding to an
integrated luminosity of 8.7 fb^{-1} collected with the
Collider Detector at Fermilab during Run II of the Tevatron.
We measure R to be 0.87±0.07, and extract the magnitude of
the top-bottom quark coupling to be |V_{tb}|=0.93±0.04,
assuming three generations of quarks. Under these
assumptions, a lower limit of |V_{tb}|>0.85(0.87) at 95%
(90%) credibility level is set.},
Doi = {10.1103/physrevlett.112.221801},
Key = {fds314168}
}
@article{fds365367,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S},
Title = {Measurement of b-quark fragmentation properties in jets
using the decay B ± → J/ψK ± in
pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {12},
Year = {2021},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2021)131},
Abstract = {The fragmentation properties of jets containing b-hadrons
are studied using charged B mesons in 139 fb−1 of pp
collisions at s = 13 TeV, recorded with the ATLAS detector
at the LHC during the period from 2015 to 2018. The B mesons
are reconstructed using the decay of B± into J/ψK±, with
the J/ψ decaying into a pair of muons. Jets are
reconstructed using the anti-kt algorithm with radius
parameter R = 0.4. The measurement determines the
longitudinal and transverse momentum profiles of the
reconstructed B hadrons with respect to the axes of the jets
to which they are geometrically associated. These
distributions are measured in intervals of the jet
transverse momentum, ranging from 50 GeV to above 100 GeV.
The results are corrected for detector effects and compared
with several Monte Carlo predictions using different parton
shower and hadronisation models. The results for the
longitudinal and transverse profiles provide useful inputs
to improve the description of heavy-flavour fragmentation in
jets. [Figure not available: see fulltext.].},
Doi = {10.1007/JHEP12(2021)131},
Key = {fds365367}
}
@article{fds308815,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari,
C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Breccia, L and Bromberg,
C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell,
M and Caner, A and Carithers, W and Carlsmith, D and Cassada, J and Castro,
A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Cropp, R and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui,
Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton,
R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi,
T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and IV,
AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin,
A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson,
C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas,
J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund,
AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu,
X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of B0-B̄0 flavor
oscillations using jet-charge and lepton flavor tagging in
pp̄ collisions at √s=1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {60},
Number = {7},
Pages = {1-22},
Year = {1999},
Abstract = {We present a measurement of the mass difference Δmd for the
B0 meson and the statistical power of the b flavor tagging
methods used. The measurement uses 90 pb-1 of data from pp̄
collisions at √s= 1.8 TeV collected with the CDF detector.
An inclusive lepton trigger is used to collect a large
sample of B hadron semileptonic decays. The mass difference
Δmd is determined from the proper time dependence of the
fraction of B hadrons that undergo flavor oscillations. The
flavor at decay is inferred from the charge of the lepton
from semileptonic B decay. The initial flavor is inferred by
determining the flavor of the other B hadron produced in the
collision, either from its semileptonic decay (soft-lepton
tag) or from its jet charge. The measurement yields
Δmd=(0.500±0.052±0.043)ℏ ps-1, where the first
uncertainty is statistical and the second uncertainty is
systematic. The statistical powers (∈D2) of the
soft-lepton and jet-charge flavor taggers are (0.91±0.10
±0.11)% and (0.78±0.12±0.08)%, respectively. ©1999 The
American Physical Society.},
Key = {fds308815}
}
@article{fds308852,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg,
C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane,
D and Cronin-Hennessy, D and Culbertson, R and Daniels, T and DeJongh,
F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L},
Title = {Measurement of bb̄ production correlations,
B0B̄0 mixing, and a limit on
∈B in pp̄ collisions at √s=1.8
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {55},
Number = {5},
Pages = {2547-2558},
Year = {1997},
Month = {March},
Abstract = {We present measurements of correlated bb̄ cross sections,
μ-μ, correlations, the average B0B̄0 mixing parameter
χ̄, and a limit on the CP-violating parameter ∈B. For
these measurements, we use muon pairs from bb double
semileptonic decays. The data used in this analysis were
taken with the Collider_Detector at Fermilab and represent
an integrated luminosity of 17.4±0.6 pb-1. The results
concerning bb̄ production correlations are compared to
predictions of next-to-leading order QCD
computations.},
Key = {fds308852}
}
@article{fds331230,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla,
G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir,
S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui,
Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton,
R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster,
M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Volobouev, I and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund,
AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu,
X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of bb̄ rapidity correlations in pp̄ collisions
at √s=1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {61},
Number = {3},
Pages = {1-18},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevD.61.032001},
Abstract = {We report the first direct measurement of bb̄ rapidity
correlations in pp̄ collisions at √=1.8 TeV. We select
events with a high transverse momentum muon accompanied by a
jet, and a second jet associated with a decay vertex
displaced from the pp̄ interaction vertex. Two independent
samples are obtained corresponding to events with a forward
(2.0<|η|<2.6) or central (|η|<0.6) muon. We
measure the ratio of forward to central bb̄ production to
be 0.361±0.033(stat)-0.031+0.015(syst), in good agreement
with the next-to-leading order QCD prediction
0.338-0.097+0.014. ©2000 The American Physical
Society.},
Doi = {10.1103/PhysRevD.61.032001},
Key = {fds331230}
}
@article{fds308462,
Author = {Aaltonen, TEA},
Title = {Measurement of branching ratio and ${B}_{s}^{0}$ lifetime in
the decay ${B}_{s}^{0}\rightarrow{J}/\psi{f}_{0}(980)$ at
{CDF}},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {5},
Pages = {052012},
Publisher = {American Physical Society},
Year = {2011},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.84.052012},
Abstract = {We present a study of Bs0 decays to the CP-odd final state
J/ψf 0(980) with J/ψ→μ+μ- and f 0(980)→π+π-. Using
pp̄ collision data with an integrated luminosity of 3.8fb-1
collected by the CDF II detector at the Tevatron we measure
a Bs0 lifetime of τ(Bs0→J/ψf0(980))=1.70-0.11+0.12(stat)±0.03(syst)
ps. This is the first measurement of the Bs0 lifetime in a
decay to a CP eigenstate and corresponds in the standard
model to the lifetime of the heavy Bs0 eigenstate. We also
measure the product of branching fractions of
Bs0→J/ψf0(980) and f0(980)→π +π- relative to the
product of branching fractions of Bs0→J/ψ and →K+K- to
be Rf0 /=0.257±0.020(stat)±0.014(syst), which is the most
precise determination of this quantity to date. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.84.052012},
Key = {fds308462}
}
@article{fds308389,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of Bs0→Ds(*)+Ds(*)- branching
ratios.},
Journal = {Physical review letters},
Volume = {108},
Number = {20},
Pages = {201801},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.201801},
Abstract = {The decays Bs0→Ds(*)+Ds(*)- are reconstructed in a data
sample corresponding to an integrated luminosity of
6.8 fb-1 collected by the CDF II detector at the
Tevatron pp[over ¯] collider. All decay modes are observed
with a significance of more than 10σ, and we measure the
Bs0 production rate times Bs0→Ds(*)+Ds(*)- branching
ratios relative to the normalization mode B0→Ds+D-to be
0.183±0.021±0.017 for Bs0→Ds+Ds-, 0.424±0.046±0.035
for Bs0→Ds*±Ds^∓, 0.654±0.072±0.065 for
Bs0→Ds*+Ds*-, and 1.261±0.095±0.112 for the inclusive
decay Bs0→Ds(*)+Ds(*)-, where the uncertainties are
statistical and systematic. These results are the most
precise single measurements to date and provide important
constraints for indirect searches for nonstandard model
physics in Bs0 mixing.},
Doi = {10.1103/physrevlett.108.201801},
Key = {fds308389}
}
@article{fds321253,
Author = {Aaltonen, T and Albrow, MG and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri,
A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher,
R},
Title = {Measurement of central exclusive π+π- production in p p ¯
collisions at s =0.9 and 1.96 TeV at CDF MEASUREMENT of
CENTRAL EXCLUSIVE π+π- ... T. AALTONEN et
al.},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.91.091101},
Abstract = {We measure exclusive π+π- production in proton-antiproton
collisions at center-of-mass energies s=0.9 and 1.96 TeV in
the Collider Detector at Fermilab. We select events with two
oppositely charged particles, assumed to be pions, with
pseudorapidity |η|<1.3 and with no other particles detected
in |η|<5.9. We require the π+π- system to have rapidity
|y|<1.0. The production mechanism of these events is
expected to be dominated by double pomeron exchange, which
constrains the quantum numbers of the central state. The
data are potentially valuable for isoscalar meson
spectroscopy and for understanding the pomeron in a region
of transition between nonperturbative and perturbative
quantum chromodynamics. The data extend up to dipion mass
M(π+π-)=5000MeV/c2 and show resonance structures
attributed to f0 and f2(1270) mesons. From the π+π- and
K+K- spectra, we place upper limits on exclusive χc0(3415)
production.},
Doi = {10.1103/PhysRevD.91.091101},
Key = {fds321253}
}
@article{fds314182,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
M},
Title = {Measurement of charged-particle spectra in Pb+Pb collisions
at √sNN = 2.76 TeV with the ATLAS detector at the
LHC},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {9},
Pages = {1-51},
Publisher = {Springer Nature},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2015)050},
Abstract = {Charged-particle spectra obtained in Pb+Pb interactions at
(Formula presented.) and pp interactions at (Formula
presented.) with the ATLAS detector at the LHC are
presented, using data with integrated luminosities of 0.15
nb−1 and 4.2 pb−1, respectively, in a wide transverse
momentum (0.5 < pT< 150 GeV) and pseudorapidity (|η| < 2)
range. For Pb+Pb collisions, the spectra are presented as a
function of collision centrality, which is determined by the
response of the forward calorimeters located on both sides
of the interaction point. The nuclear modification factors
RAA and RCP are presented in detail as a function of
centrality, pT and η. They show a distinct pT-dependence
with a pronounced minimum at about 7 GeV. Above 60 GeV, RAA
is consistent with a plateau at a centrality-dependent
value, within the uncertainties. The value is 0.55 ±
0.01(stat.) ± 0.04(syst.) in the most central collisions.
The RAA distribution is consistent with flat |η| dependence
over the whole transverse momentum range in all centrality
classes.},
Doi = {10.1007/JHEP09(2015)050},
Key = {fds314182}
}
@article{fds316656,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of colour flow with the jet pull angle in tt-
events using the ATLAS detector at √s=8
TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {750},
Pages = {475-493},
Publisher = {Elsevier BV},
Year = {2015},
Month = {November},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2015.09.051},
Abstract = {The distribution and orientation of energy inside jets is
predicted to be an experimental handle on colour connections
between the hard-scatter quarks and gluons initiating the
jets. This Letter presents a measurement of the distribution
of one such variable, the jet pull angle. The pull angle is
measured for jets produced in tt- events with one W boson
decaying leptonically and the other decaying to jets using
20.3 fb-1 of data recorded with the ATLAS detector at a
centre-of-mass energy of s=8 TeV at the LHC. The jet pull
angle distribution is corrected for detector resolution and
acceptance effects and is compared to various
models.},
Doi = {10.1016/j.physletb.2015.09.051},
Key = {fds316656}
}
@article{fds308885,
Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cen, Y},
Title = {Measurement of correlated micro-b-bar jet cross sections in
pp-bar collisions at s=1.8 TeV.},
Journal = {Physical review. D, Particles and fields},
Volume = {53},
Number = {3},
Pages = {1051-1065},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevd.53.1051},
Abstract = {We report on measurements of differential µ-b- cross
sections, where the muon is from a semileptonic b decay and
the b- is identified using precision track reconstruction in
jets. The semidifferential correlated cross sections
dσ/(formula presented), and dσ/dδφ(µ-b-) for (formula
presented) 10 GeV, (formula presented)<1.5 are presented and
compared to next-to-leading order QCD calculations. © 1996
The American Physical Society.},
Doi = {10.1103/physrevd.53.1051},
Key = {fds308885}
}
@article{fds308410,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Measurement of CP-violating asymmetries in D0→π
+π - and D0→K +K
- decays at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012009},
Abstract = {We report on a measurement of CP-violating asymmetries (A
CP) in the Cabibbo-suppressed D0→π +π - and D0→K +K -
decays reconstructed in a data sample corresponding to 5.9fb
-1 of integrated luminosity collected by the upgraded
Collider Detector at Fermilab. We use the strong decay D
*+→D0π + to identify the flavor of the charmed meson at
production and exploit CP-conserving strong cc̄ pair
production in pp̄ collisions. High-statistics samples of
Cabibbo-favored D0→K -π + decays with and without a D *±
tag are used to correct for instrumental effects and
significantly reduce systematic uncertainties. We measure A
CP(D0→π +π -)=(+0.22±0.24(stat) ±0.11(syst))% and A
CP(D0→K +K -)=(-0.24±0.22(stat)±0.09(syst))%, in
agreement with CP conservation. These are the most precise
determinations from a single experiment to date. Under the
assumption of negligible direct CP violation in D0→π +π
- and D0→K +K - decays, the results provide an upper limit
to the CP-violating asymmetry in D0 mixing,
|ACPind(D0)|<0.13% at the 90% confidence level. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.85.012009},
Key = {fds308410}
}
@article{fds308421,
Author = {Aaltonen, T and Ãlvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and D'Errico, M},
Title = {Measurement of CP-violation asymmetries in D0→KS0π
+π -},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.86.032007},
Abstract = {We report a measurement of time-integrated CP-violation
asymmetries in the resonant substructure of the three-body
decay D0→KS0π +π - using CDF II data corresponding to
6.0fb -1 of integrated luminosity from Tevatron pp̄
collisions at √s=1.96TeV. The charm mesons used in this
analysis come from D *+(2010) →D0π + and D *-(2010)→D
̄0π -, where the production flavor of the charm meson is
determined by the charge of the accompanying pion. We apply
a Dalitz-amplitude analysis for the description of the
dynamic decay structure and use two complementary
approaches, namely, a full Dalitz-plot fit employing the
isobar model for the contributing resonances and a
model-independent bin-by-bin comparison of the D0 and D ̄0
Dalitz plots. We find no CP-violation effects and measure an
asymmetry of A CP=(-0.05±0. 57(stat)±0.54(syst))% for the
overall integrated CP-violation asymmetry, consistent with
the standard model prediction. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.032007},
Key = {fds308421}
}
@article{fds308570,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and González, BAL and Amerio,
S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D},
Title = {Measurement of cross sections for b jet production in events
with a Z boson in pp̄ collisions at s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.79.052008},
Abstract = {A measurement of the b jet production cross section is
presented for events containing a Z boson produced in pp̄
collisions at s=1.96TeV, using data corresponding to an
integrated luminosity of 2fb-1 collected by the CDF II
detector at the Tevatron. Z bosons are selected in the
electron and muon decay modes. Jets are considered with
transverse energy ET>20GeV and pseudorapidity |η|<1.5 and
are identified as b jets using a secondary vertex algorithm.
The ratio of the integrated Z+b jet cross section to the
inclusive Z production cross section is measured to be
3.32±0.53(stat)±0.42(syst) ×10-3. This ratio is also
measured differentially in jet ET, jet η, Z-boson
transverse momentum, number of jets, and number of b jets.
The predictions from leading-order Monte Carlo generators
and next-to-leading-order QCD calculations are found to be
consistent with the measurements within experimental and
theoretical uncertainties. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevD.79.052008},
Key = {fds308570}
}
@article{fds375938,
Author = {Jackson, P and Kong, AXY and Oliver, JL and Ruggeri, TA and Sharma, AS and White, MJ and Jain, V and Swift, SP and Gingrich, DM and Pinfold, JL and Wang, H and Cakir, O and Duran Yildiz and H and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Belfkir, M and Berger, N and Costanza, F and Cueto, A and Dartsi, O and Delmastro, M and Di Ciaccio,
L and Franco, L and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo
Martinez, N and Portales, L and Sauvan, E and Wingerter-Seez, I and Abulaiti, Y and Benjamin, DP and Bhopatkar, VS and Chekanov, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe,
J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Zhang, J and Berlendis, S and Cheu, E and Delitzsch, CM and Johns, KA and Lampl, W and LeBlanc, M and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave,
B and De, K and Eifert, T and Farbin, A and Hadavand, HK and Little, JD and Ozturk, N and Usai, G and White, A and Angelidakis, S and Bellos, P and Fassouliotis, D and Gkialas, I and Kourkoumelis, C and Papageorgiou,
K and Alexopoulos, T and Bakalis, C and Benekos, N and Gazis, EN and Gkountoumis, P and Kitsaki, C and Koulouris, A and Maltezos, S and Paraskevopoulos, C and Zacharis, G and Andeen, T and Burton, CD and Choi, K and Nikiforou, N and Onyisi, PUE and Potti, H and Roy, A and Unal,
M and Webb, AF and Beddall, AJ and Celebi, E and Cetin,
SA},
Title = {Measurement of cross sections for production of a Z boson in
association with a flavor-inclusive or doubly b-tagged
large-radius jet in proton-proton collisions at √s = 13
TeV with the ATLAS experiment},
Journal = {Physical Review D},
Volume = {108},
Number = {1},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.108.012022},
Abstract = {We present measurements of cross sections for production of
a leptonically decaying Z boson in association with a
large-radius jet in 13 TeV proton-proton collisions at the
LHC, using 36 fb - 1 of data from the ATLAS detector.
Integrated and differential cross sections are measured at
particle level in both a flavor inclusive and a doubly b
-tagged fiducial phase space. The large-radius jet mass and
transverse momentum, its kinematic relationship to the Z
boson, and the angular separation of b -tagged small-radius
track jets within the large-radius jet are measured. This
measurement constitutes an important test of perturbative
quantum chromodynamics in kinematic and flavor
configurations relevant to several Higgs boson and
beyond-Standard-Model physics analyses. The results
highlight issues with modeling of additional hadronic
activity in the flavor-inclusive selection, and a
distinction between flavor-number schemes in the b -tagged
phase space.},
Doi = {10.1103/PhysRevD.108.012022},
Key = {fds375938}
}
@article{fds308787,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and de
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson,
R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin,
T and Dittmann, JR and Dominguez, A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Erbacher, R and Errede, D and Errede, S and Fan, Q and Feild,
RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman,
J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov, I and Goshaw,
AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Guimaraes da Costa and J and Haas, RM and Haber, C and Hahn, SR and Hall,
C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser,
J and Heinrich, J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon,
T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim,
MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Lee, AM and Lee, K and Leone, S and Lewis,
JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima,
K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JA and Mayer, J and Mazzanti,
P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CY and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Roy,
A and Ruiz, A and Safonov, A and St Denis and R and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt,
M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel,
S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding,
J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda,
H and Trischuk, W and de Troconiz, JF and Tseng, J and Turini, N and Ukegawa, F and Vaiciulis, T and Valls, J and Vejcik, S and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and von
der Mey, M and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson,
P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh,
P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S and CDF Collaboration},
Title = {Measurement of d sigma/dM and forward-backward charge
asymmetry for high-mass Drell-Yan e(+)e(-) pairs from pp
macro collisions at square root of s = 1.8
TeV.},
Journal = {Physical review letters},
Volume = {87},
Number = {13},
Pages = {131802},
Year = {2001},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.87.131802},
Abstract = {We report on a measurement of the mass dependence of the
forward-backward charge asymmetry, A(FB), and production
cross section d sigma/dM for e(+)e(-) pairs with mass
M(ee)>40 GeV/c(2). The data sample consists of 108 pb(-1) of
pp macro collisions at square root of s = 1.8 TeV taken by
the Collider Detector at Fermilab during 1992-1995. The
measured asymmetry and d sigma/dM are compared with the
predictions of the standard model and a model with an extra
Z' gauge boson.},
Doi = {10.1103/physrevlett.87.131802},
Key = {fds308787}
}
@article{fds315957,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of D⁎±, D± and
Ds± meson production cross sections
in pp collisions at √s=7 TeV with the ATLAS
detector},
Journal = {Nuclear Physics B},
Volume = {907},
Pages = {717-763},
Publisher = {Elsevier BV},
Year = {2016},
Month = {June},
ISSN = {0550-3213},
url = {http://dx.doi.org/10.1016/j.nuclphysb.2016.04.032},
Abstract = {The production of D⁎±, D± and Ds± charmed mesons has
been measured with the ATLAS detector in pp collisions at
s=7 TeV at the LHC, using data corresponding to an
integrated luminosity of 280 nb−1. The charmed mesons have
been reconstructed in the range of transverse momentum
3.5<pT(D)<100 GeV and pseudorapidity |η(D)|<2.1. The
differential cross sections as a function of transverse
momentum and pseudorapidity were measured for D⁎± and D±
production. The next-to-leading-order QCD predictions are
consistent with the data in the visible kinematic region
within the large theoretical uncertainties. Using the
visible D cross sections and an extrapolation to the full
kinematic phase space, the strangeness-suppression factor in
charm fragmentation, the fraction of charged non-strange D
mesons produced in a vector state, and the total cross
section of charm production at s=7 TeV were
derived.},
Doi = {10.1016/j.nuclphysb.2016.04.032},
Key = {fds315957}
}
@article{fds321226,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of differential J/ψ production cross sections
and forward-backward ratios in p + Pb collisions with the
ATLAS detector},
Journal = {Physical Review C - Nuclear Physics},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevC.92.034904},
Abstract = {Measurements of differential cross sections for J/ψ
production in p + Pb collisions at (√SNN at the CERN Large
Hadron Collider with the ATLAS detector are presented. The
data set used corresponds to an integrated luminosity of
28.1 nb−1. The J/ψ mesons are reconstructed in the dimuon
decay channel over the transverse momentum range 8 < pT < 30
GeV and over the center-of-mass rapidity range −2.87 <
y∗ < 1.94. Prompt J/ψ are separated from J/ψ resulting
from b-hadron decays through an analysis of the distance
between the J/ψ decay vertex and the event primary vertex.
The differential cross section for production of nonprompt
J/ψ is compared to a FONLL calculation that does not
include nuclear effects. Forward-backward production ratios
are presented and compared to theoretical predictions. These
results complement previously published results by covering
a region of higher transverse momentum and more central
rapidity. They thus constrain the kinematic dependence of
nuclear modifications of charmonium and b-quark production
in p + Pb collisions.},
Doi = {10.1103/PhysRevC.92.034904},
Key = {fds321226}
}
@article{fds321278,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JJA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of differential production cross sections for Z
/γ∗ bosons in association with jets in p p ¯ collisions
at s =1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.91.012002},
Abstract = {Differential cross sections for the production of Z bosons
or off-shell photons γ∗ in association with jets are
measured in proton-antiproton collisions at center-of-mass
energy s=1.96TeV using the full data set collected with the
Collider Detector at Fermilab in Tevatron run II and
corresponding to 9.6fb-1 of integrated luminosity. Results
include first measurements at CDF of differential cross
sections in events with a Z/γ∗ boson and three or more
jets, the inclusive cross section for production of Z/γ∗
and four or more jets, and cross sections as functions of
various angular observables in lower jet-multiplicity final
states. Measured cross sections are compared to several
theoretical predictions.},
Doi = {10.1103/PhysRevD.91.012002},
Key = {fds321278}
}
@article{fds321327,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of differential production cross-sections for a
Z boson in association with b-jets in 7 TeV proton-proton
collisions with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {10},
Pages = {1-49},
Publisher = {Springer Nature},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2014)141},
Abstract = {Abstract: Measurements of differential production
cross-sections of a Z boson in association with b-jets in pp
collisions at √ = 7 TeV are reported. The data analysed
correspond to an integrated luminosity of 4.6 fb−1
recorded with the ATLAS detector at the Large Hadron
Collider. Particle-level cross-sections are determined for
events with a Z boson decaying into an electron or muon
pair, and containing b-jets. For events with at least one
b-jet, the cross-section is presented as a function of the Z
boson transverse momentum and rapidity, together with the
inclusive b-jet cross-section as a function of b-jet
transverse momentum, rapidity and angular separations
between the b-jet and the Z boson. For events with at least
two b-jets, the cross-section is determined as a function of
the invariant mass and angular separation of the two highest
transverse momentum b-jets, and as a function of the Z boson
transverse momentum and rapidity. Results are compared to
leading-order and next-to-leading-order perturbative QCD
calculations.},
Doi = {10.1007/JHEP10(2014)141},
Key = {fds321327}
}
@article{fds308866,
Author = {al, FAE},
Title = {Measurement of diffractive dijet production at the Fermilab
Tevatron},
Journal = {Phys. Rev. Lett.},
Volume = {79},
Number = {14},
Pages = {2636-2641},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.2636},
Abstract = {We report the observation and measurement of the rate of
diffractive dijet production at the Fermilab Tevatron p¯p
collider at √s=1.8TeV. In events with two jets of
ET>20GeV, 1.8<|η|<3.5, and η1η2>0, we find that the
diffractive to nondiffractive production ratio is
RJJ=[0.75±0.05(stat)±0.09(syst)]%. By comparing this
result, in combination with our measured rate for
diffractive W boson production reported previously, with
predictions based on a hard partonic pomeron structure, we
determine the pomeron gluon fraction to be fg=0.7±0.2. ©
1997 American Physical Society.},
Doi = {10.1103/PhysRevLett.79.2636},
Key = {fds308866}
}
@article{fds330269,
Author = {al, FAE},
Title = {Measurement of Dijet angular distributions by the Collider
Detector at Fermilab},
Journal = {Phys. Rev. Lett.},
Volume = {77},
Number = {27},
Pages = {5336-5341},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevLett.77.5336},
Abstract = {We have used 106pb of data collected in pp collisions at
√s = 1.8 TeV by the Collider Detector at Fermilab to
measure jet angular distributions in events with two jets in
the final state. The angular distributions agree with next
to leading order predictions of QCD in all dijet invariant
mass regions. The data exclude at 95% CL a model of quark
substructure in which only up and down quarks are composite
and the contact interaction scale is ⩘ ≤1.6 TeV or ⩘
≤1.4 TeV. For a model in which all quarks are composite
the excluded regions are ⩘ ≤1.8 TeV and ⩘ ≤1.6 TeV.
© 1996 The American Physical Society. -1 + - + - ud
ud},
Doi = {10.1103/PhysRevLett.77.5336},
Key = {fds330269}
}
@article{fds321352,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
JF},
Title = {Measurement of dijet cross-sections in pp collisions at 7
TeV centre-of-mass energy using the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {5},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP05(2014)059},
Abstract = {Double-differential dijet cross-sections measured in pp
collisions at the LHC with a 7TeV centre-of-mass energy are
presented as functions of dijet mass and half the rapidity
separation of the two highest-pT jets. These measurements
are obtained using data corresponding to an integrated
luminosity of 4.5 fb−1, recorded by the ATLAS detector in
2011. The data are corrected for detector effects so that
cross-sections are presented at the particle level.
Cross-sections are measured up to 5TeV dijet mass using jets
reconstructed with the anti-kt algorithm for values of the
jet radius parameter of 0.4 and 0.6. The cross-sections are
compared with next-to-leading-order perturbative QCD
calculations by NLOJet++ corrected to account for
non-perturbative effects. Comparisons with POWHEG
predictions, using a next-to-leading-order matrix element
calculation interfaced to a partonshower Monte Carlo
simulation, are also shown. Electroweak effects are
accounted for in both cases. The quantitative comparison of
data and theoretical predictions obtained using various
parameterizations of the parton distribution functions is
performed using a frequentist method. In general, good
agreement with data is observed for the NLOJet++ theoretical
predictions when using the CT10, NNPDF2.1 and MSTW 2008 PDF
sets. Disagreement is observed when using the ABM11 and
HERAPDF1.5 PDF sets for some ranges of dijet mass and half
the rapidity separation. An example setting a lower limit on
the compositeness scale for a model of contact interactions
is presented, showing that the unfolded results can be used
to constrain contributions to dijet production beyond that
predicted by the Standard Model.},
Doi = {10.1007/JHEP05(2014)059},
Key = {fds321352}
}
@article{fds321362,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Measurement of distributions sensitive to the underlying
event in inclusive Z-boson production in [Formula: see text]
collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {12},
Pages = {3195},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3195-6},
Abstract = {A measurement of charged-particle distributions sensitive to
the properties of the underlying event is presented for an
inclusive sample of events containing a [Formula: see
text]-boson, decaying to an electron or muon pair. The
measurement is based on data collected using the ATLAS
detector at the LHC in proton-proton collisions at a
centre-of-mass energy of [Formula: see text] TeV with an
integrated luminosity of [Formula: see text] fb[Formula:
see text]. Distributions of the charged particle
multiplicity and of the charged particle transverse momentum
are measured in regions of azimuthal angle defined with
respect to the [Formula: see text]-boson direction. The
measured distributions are compared to similar distributions
measured in jet events, and to the predictions of various
Monte Carlo generators implementing different underlying
event models.},
Doi = {10.1140/epjc/s10052-014-3195-6},
Key = {fds321362}
}
@article{fds308864,
Author = {al, FAE},
Title = {Measurement of double parton scattering in (p)over-bar-p
collisions at root s=1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {79},
Number = {4},
Pages = {584-589},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.79.584},
Abstract = {A strong signal for double parton scattering (DP) is
observed in a 16 pb-1 sample of p̄ p → γ + 3 jets + X
data from the CDF experiment at the Fermilab Tevatron. The
process-independent DP parameter, σeff, is obtained without
reference to theoretical calculations by comparing observed
DP events to events with hard scatterings at separate p̄ p
collisions. The result, σeff = (14.5 ± 1.7-2.3+1.7) mb,
represents a significant improvement over previous
measurements. For the first time, the Feynman x dependence
of the σeff parameter is investigated, and no dependence is
seen.},
Doi = {10.1103/physrevlett.79.584},
Key = {fds308864}
}
@article{fds308865,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi Bacchetta and P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro Galtieri and A and Barnes, VE and Barnett, BA and Barone, M and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas,
A and Berge, JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner,
N and Buckley Geer and E and Budd, HS and Burkett, K and Busetto, G and Byon
Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell,
M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou,
CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca,
E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cronin Hennessy and D and Culbertson,
R and Daniels, T and De Jongh and F and Delchamps, S and Dell Agnello and S and Dell Orso and M and Demina, R and Demortier, L},
Title = {Measurement of double parton scattering in pp collisons at
s},
Journal = {Physical Review Letters},
Volume = {79},
Number = {4},
Pages = {578-583},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.584},
Abstract = {A strong signal for double parton scattering (DP) is
observed in a 16 pb−1 sample of pp → γ + 3 jets + X
data from the CDF experiment at the Fermilab Tevatron. The
process-independent DP parameter, σ eff, is obtained
without reference to theoretical calculations by comparing
observed DP events to events with hard scatterings at
separate pp collisons. The result, σ eff = (14.5 ± 1.7
+1.7−2.3)mb, represents a significant improvement over
previous measurements. For the first time, the Feynman x
dependence of the σeff parameter is investigated, and no
dependence is seen. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.79.584},
Key = {fds308865}
}
@article{fds308497,
Author = {Aaltonen, T and Adelman, J and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, J and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway,
J},
Title = {Measurement of dσ/dy of Drell-Yan e+e-
pairs in the Z mass region from pp̄ collisions at √s=1.96
TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {692},
Number = {4},
Pages = {232-239},
Publisher = {Elsevier BV},
Year = {2010},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2010.06.043},
Abstract = {We report on a CDF measurement of the total cross section
and rapidity distribution, dσ/dy, for γ*Z→e+e- events in
the Z boson mass region (66<Mee<116 GeV/c2) produced in pp-
collisions at s=1.96 TeV with 2.1 fb-1 of integrated
luminosity. The measured cross section of 257±16 pb and
dσ/dy distribution are compared with Next-to-Leading-Order
(NLO) and Next-to-Next-to-Leading-Order (NNLO) QCD theory
predictions with CTEQ and MRST/MSTW parton distribution
functions (PDFs). There is good agreement between the
experimental total cross section and dσ/dy measurements
with theoretical calculations with the most recent NNLO
PDFs. © 2010 Elsevier B.V.},
Doi = {10.1016/j.physletb.2010.06.043},
Key = {fds308497}
}
@article{fds308459,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of event shapes in $p\overline{p}$ collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {11},
Pages = {112007},
Publisher = {American Physical Society},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.83.112007},
Abstract = {A study of event-shape observables in proton-antiproton
collisions at √s=1.96TeV is presented. The data for this
analysis were recorded by the CDF II Detector at the
Tevatron Collider. The variables studied are the transverse
thrust and thrust minor, both defined in the plane
perpendicular to the beam direction. The observables are
measured using energies from unclustered calorimeter cells.
In addition to studies of the differential distributions, we
present the dependence of event-shape mean values on the
leading-jet transverse energy. Data are compared with pythia
Tune A and to resummed parton-level predictions that were
matched to fixed-order results at next-to-leading-order
(NLO) accuracy (NLO+NLL). Predictions from pythia Tune A
agree fairly well with the data. However, the underlying
event contributes significantly to these observables, making
it difficult to make direct comparisons to the NLO+NLL
predictions, which do not account for the underlying event.
To overcome this difficulty, we introduce a new observable,
a weighted difference of the mean values of the thrust and
thrust minor, which is less sensitive to the underlying
event, allowing for a comparison with NLO+NLL. Both pythia
Tune A and the NLO+NLL calculations agree well within the
20% theoretical uncertainty with the data for this
observable, indicating that perturbative QCD successfully
describes shapes of the hadronic final states. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.83.112007},
Key = {fds308459}
}
@article{fds321342,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O and Arnal, V},
Title = {Measurement of event-plane correlations in √sNN
= 2.76 TeV lead-lead collisions with the ATLAS
detector},
Journal = {Physical Review C - Nuclear Physics},
Volume = {90},
Number = {2},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevC.90.024905},
Abstract = {A measurement of event-plane correlations involving two or
three event planes of different order is presented as a
function of centrality for 7 μb-1 Pb+Pb collision data at
sNN=2.76 TeV, recorded by the ATLAS experiment at the Large
Hadron Collider. Fourteen correlators are measured using a
standard event-plane method and a scalar-product method, and
the latter method is found to give a systematically larger
correlation signal. Several different trends in the
centrality dependence of these correlators are observed.
These trends are not reproduced by predictions based on the
Glauber model, which includes only the correlations from the
collision geometry in the initial state. Calculations that
include the final-state collective dynamics are able to
describe qualitatively, and in some cases also
quantitatively, the centrality dependence of the measured
correlators. These observations suggest that both the
fluctuations in the initial geometry and the nonlinear
mixing between different harmonics in the final state are
important for creating these correlations in momentum
space.},
Doi = {10.1103/PhysRevC.90.024905},
Key = {fds321342}
}
@article{fds321187,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
Title = {Measurement of event-shape observables in [Formula: see
text] events in pp collisions at [Formula: see
text] [Formula: see text] with the ATLAS detector at the
LHC.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {7},
Pages = {375},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4176-8},
Abstract = {Event-shape observables measured using charged particles in
inclusive <i>Z</i>-boson events are presented, using the
electron and muon decay modes of the <i>Z</i> bosons. The
measurements are based on an integrated luminosity of
[Formula: see text] of proton-proton collisions recorded by
the ATLAS detector at the LHC at a centre-of-mass energy
[Formula: see text] [Formula: see text]. Charged-particle
distributions, excluding the lepton-antilepton pair from the
<i>Z</i>-boson decay, are measured in different ranges of
transverse momentum of the <i>Z</i> boson. Distributions
include multiplicity, scalar sum of transverse momenta, beam
thrust, transverse thrust, spherocity, and [Formula: see
text]-parameter, which are in particular sensitive to
properties of the underlying event at small values of the
<i>Z</i>-boson transverse momentum. The measured observables
are compared with predictions from Pythia 8, Sherpa, and
Herwig 7. Typically, all three Monte Carlo generators
provide predictions that are in better agreement with the
data at high <i>Z</i>-boson transverse momenta than at low
<i>Z</i>-boson transverse momenta, and for the observables
that are less sensitive to the number of charged particles
in the event.},
Doi = {10.1140/epjc/s10052-016-4176-8},
Key = {fds321187}
}
@article{fds375934,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Measurement of exclusive pion pair production in
proton–proton collisions at √s=7TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11700-x},
Abstract = {The exclusive production of pion pairs in the process pp→
ppπ+π- has been measured at s=7TeV with the ATLAS detector
at the LHC, using 80μb-1 of low-luminosity data. The pion
pairs were detected in the ATLAS central detector while
outgoing protons were measured in the forward ATLAS ALFA
detector system. This represents the first use of proton
tagging to measure an exclusive hadronic final state at the
LHC. A cross-section measurement is performed in two
kinematic regions defined by the proton momenta, the pion
rapidities and transverse momenta, and the pion–pion
invariant mass. Cross-section values of 4.8±1.0(stat)-0.2+0.3(syst)μb
and 9±6(stat)-2+2(syst)μb are obtained in the two regions;
they are compared with theoretical models and provide a
demonstration of the feasibility of measurements of this
type.},
Doi = {10.1140/epjc/s10052-023-11700-x},
Key = {fds375934}
}
@article{fds321185,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of exclusive γγ →w+W- production and search
for exclusive Higgs boson production in pp collisions at s
=8 TeV using the ATLAS detector},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.032011},
Abstract = {Searches for exclusively produced W boson pairs in the
process pp(γγ)→pW+W-p and an exclusively produced Higgs
boson in the process pp(gg)→pHp have been performed using
e±μ final states. These measurements use 20.2 fb-1 of pp
collisions collected by the ATLAS experiment at a
center-of-mass energy s=8 TeV at the LHC. Exclusive
production of W+W- consistent with the Standard Model
prediction is found with 3.0σ significance. The exclusive
W+W- production cross section is determined to be
σ(γγ→W+W-→e±μX)=6.9±2.2(stat)±1.4(sys) fb, in
agreement with the Standard Model prediction. Limits on
anomalous quartic gauge couplings are set at 95% confidence
level as -1.7×10-6<a0W/Λ2<1.7×10-6 GeV-2 and
-6.4×10-6<aCW/Λ2<6.3×10-6 GeV-2. A 95% confidence-level
upper limit on the total production cross section for an
exclusive Higgs boson is set to 1.2 pb.},
Doi = {10.1103/PhysRevD.94.032011},
Key = {fds321185}
}
@article{fds321218,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of exclusive γγ→ℓ+ℓ−
production in proton–proton collisions at √s=7 TeV with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {749},
Pages = {242-261},
Publisher = {Elsevier BV},
Year = {2015},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2015.07.069},
Abstract = {This Letter reports a measurement of the exclusive
γγ→ℓ+ℓ− (ℓ=e, μ) cross-section in
proton–proton collisions at a centre-of-mass energy of 7
TeV by the ATLAS experiment at the LHC, based on an
integrated luminosity of 4.6 fb−1. For the electron or
muon pairs satisfying exclusive selection criteria, a fit to
the dilepton acoplanarity distribution is used to extract
the fiducial cross-sections. The cross-section in the
electron channel is determined to be σγγ→e+e−excl.=0.428
± 0.035 (stat.) ± 0.018 (syst.) pb for a phase–space
region with invariant mass of the electron pairs greater
than 24 GeV, in which both electrons have transverse
momentum pT>12 GeV and pseudorapidity |η|<2.4. For muon
pairs with invariant mass greater than 20 GeV, muon
transverse momentum pT>10 GeV and pseudorapidity |η|<2.4,
the cross-section is determined to be σγγ→μ+μ−excl.=0.628
± 0.032 (stat.) ± 0.021 (syst.) pb. When proton absorptive
effects due to the finite size of the proton are taken into
account in the theory calculation, the measured
cross-sections are found to be consistent with the theory
prediction.},
Doi = {10.1016/j.physletb.2015.07.069},
Key = {fds321218}
}
@article{fds321178,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Measurement of fiducial differential cross sections of
gluon-fusion production of Higgs bosons decaying to WW
∗→eνμν with the ATLAS detector at √s=8
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)104},
Abstract = {This paper describes a measurement of fiducial and
differential cross sections of gluon-fusion Higgs boson
production in the H → W W∗→ eνμν channel, using
20.3 fb−1 of proton-proton collision data. The data were
produced at a centre-of-mass energy of s=8 TeV at the CERN
Large Hadron Collider and recorded by the ATLAS detector in
2012. Cross sections are measured from the observed H→ W
W∗→ eνμν signal yield in categories distinguished by
the number of associated jets. The total cross section is
measured in a fiducial region defined by the kinematic
properties of the charged leptons and neutrinos.
Differential cross sections are reported as a function of
the number of jets, the Higgs boson transverse momentum, the
dilepton rapidity, and the transverse momentum of the
leading jet. The jet-veto efficiency, or fraction of events
with no jets above a given transverse momentum threshold, is
also reported. All measurements are compared to QCD
predictions from Monte Carlo generators and fixed-order
calculations, and are in agreement with the Standard Model
predictions.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP08(2016)104},
Key = {fds321178}
}
@article{fds321367,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Measurement of flow harmonics with multi-particle cumulants
in Pb+Pb collisions at [Formula: see text] TeV with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {11},
Pages = {3157},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3157-z},
Abstract = {ATLAS measurements of the azimuthal anisotropy in lead-lead
collisions at [Formula: see text] TeV are shown using a
dataset of approximately 7 [Formula: see text]b[Formula:
see text] collected at the LHC in 2010. The measurements are
performed for charged particles with transverse momenta
[Formula: see text] GeV and in the pseudorapidity range
[Formula: see text]. The anisotropy is characterized by the
Fourier coefficients, [Formula: see text], of the
charged-particle azimuthal angle distribution for [Formula:
see text]-4. The Fourier coefficients are evaluated using
multi-particle cumulants calculated with the generating
function method. Results on the transverse momentum,
pseudorapidity and centrality dependence of the [Formula:
see text] coefficients are presented. The elliptic flow,
[Formula: see text], is obtained from the two-, four-, six-
and eight-particle cumulants while higher-order
coefficients, [Formula: see text] and [Formula: see text],
are determined with two- and four-particle cumulants. Flow
harmonics [Formula: see text] measured with four-particle
cumulants are significantly reduced compared to the
measurement involving two-particle cumulants. A comparison
to [Formula: see text] measurements obtained using different
analysis methods and previously reported by the LHC
experiments is also shown. Results of measurements of flow
fluctuations evaluated with multi-particle cumulants are
shown as a function of transverse momentum and the collision
centrality. Models of the initial spatial geometry and its
fluctuations fail to describe the flow fluctuations
measurements.},
Doi = {10.1140/epjc/s10052-014-3157-z},
Key = {fds321367}
}
@article{fds321215,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of four-jet differential cross sections in
√s=8 TeV proton-proton collisions using the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {12},
Pages = {1-76},
Publisher = {Springer Nature},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2015)105},
Abstract = {Differential cross sections for the production of at least
four jets have been measured in proton-proton collisions at
(Formula presented.) TeV at the Large Hadron Collider using
the ATLAS detector. Events are selected if the four anti-ktR
= 0.4 jets with the largest transverse momentum (pT) within
the rapidity range |y| < 2.8 are well separated (ΔR4jmin >
0.65), all have pT > 64 GeV, and include at least one jet
with pT > 100 GeV. The dataset corresponds to an integrated
luminosity of 20.3 fb−1. The cross sections, corrected for
detector effects, are compared to leading-order and
next-to-leading-order calculations as a function of the jet
momenta, invariant masses, minimum and maximum opening
angles and other kinematic variables.},
Doi = {10.1007/JHEP12(2015)105},
Key = {fds321215}
}
@article{fds365417,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Measurement of hadronic event shapes in high-p T
multijet final states at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {1},
Year = {2021},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2021)188},
Abstract = {A measurement of event-shape variables in proton-proton
collisions at large momentum transfer is presented using
data collected at s = 13 TeV with the ATLAS detector at the
Large Hadron Collider. Six event-shape variables calculated
using hadronic jets are studied in inclusive multijet events
using data corresponding to an integrated luminosity of 139
fb−1. Measurements are performed in bins of jet
multiplicity and in different ranges of the scalar sum of
the transverse momenta of the two leading jets, reaching
scales beyond 2 TeV. These measurements are compared with
predictions from Monte Carlo event generators containing
leading-order or next-to-leading order matrix elements
matched to parton showers simulated to leading-logarithm
accuracy. At low jet multiplicities, shape discrepancies
between the measurements and the Monte Carlo predictions are
observed. At high jet multiplicities, the shapes are better
described but discrepancies in the normalisation are
observed. [Figure not available: see fulltext.]},
Doi = {10.1007/JHEP01(2021)188},
Key = {fds365417}
}
@article{fds321311,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H},
Title = {Measurement of Higgs boson production in the diphoton decay
channel in pp collisions at center-of-mass energies of 7 and
8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.90.112015},
Abstract = {A measurement of the production processes of the recently
discovered Higgs boson is performed in the two-photon final
state using 4.5 fb-1of proton-proton collisions data at √s
= 7 TeV and 20.3 fb-1at √s = 8 TeV collected by the ATLAS
detector at the Large Hadron Collider. The number of
observed Higgs boson decays to diphotons divided by the
corresponding Standard Model prediction, called the signal
strength, is found to be μ = 1.17 ± 0.27 at the value of
the Higgs boson mass measured by ATLAS, mH= 125.4 GeV. The
analysis is optimized to measure the signal strengths for
individual Higgs boson production processes at this value of
mH. They are found to be μggF= 1.32 ± 0.38, μVBF= 0.8 ±
0.7, μWH= 1.0 ± 1.6, μZH= 0.1+3.7-0.1, and μtt¯H=
1.6+2.7-1.8, for Higgs boson production through gluon
fusion, vector-boson fusion, and in association with a W or
Z boson or a top-quark pair, respectively. Compared with the
previously published ATLAS analysis, the results reported
here also benefit from a new energy calibration procedure
for photons and the subsequent reduction of the systematic
uncertainty on the diphoton mass resolution. No significant
deviations from the predictions of the Standard Model are
found.},
Doi = {10.1103/PhysRevD.90.112015},
Key = {fds321311}
}
@article{fds329810,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Measurement of inclusive and differential cross sections in
the H → ZZ * → 4ℓ decay channel in pp
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {10},
Publisher = {Springer Nature},
Year = {2017},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2017)132},
Abstract = {Inclusive and differential fiducial cross sections of Higgs
boson production in proton-proton collisions are measured in
the H → ZZ* → 4ℓ decay channel. The proton-proton
collision data were produced at the Large Hadron Collider at
a centre-of-mass energy of 13 TeV and recorded by the ATLAS
detector in 2015 and 2016, corresponding to an integrated
luminosity of 36.1 fb−1. The inclusive fiducial cross
section in the H → ZZ* → 4ℓ decay channel is measured
to be 3.62 ± 0.50(stat)− 0.20+ 0.25 (sys) fb, in
agreement with the Standard Model prediction of 2.91 ± 0.13
fb. The cross section is also extrapolated to the total
phase space including all Standard Model Higgs boson decays.
Several differential fiducial cross sections are measured
for observables sensitive to the Higgs boson production and
decay, including kinematic distributions of jets produced in
association with the Higgs boson. Good agreement is found
between data and Standard Model predictions. The results are
used to put constraints on anomalous Higgs boson
interactions with Standard Model particles, using the
pseudo-observable extension to the kappa-framework.[Figure
not available: see fulltext.].},
Doi = {10.1007/JHEP10(2017)132},
Key = {fds329810}
}
@article{fds314175,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurement of inclusive jet charged-particle fragmentation
functions in Pb+Pb collisions at √sNN=2.76 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {739},
Pages = {320-342},
Publisher = {Elsevier BV},
Year = {2014},
Month = {December},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2014.10.065},
Abstract = {Measurements of charged-particle fragmentation functions of
jets produced in ultra-relativistic nuclear collisions can
provide insight into the modification of parton showers in
the hot, dense medium created in the collisions. ATLAS has
measured jets in sNN=2.76 TeV Pb+Pb collisions at the LHC
using a data set recorded in 2011 with an integrated
luminosity of 0.14 nb−1. Jets were reconstructed using the
anti-kt algorithm with distance parameter values
R=0.2,0.3,and 0.4. Distributions of charged-particle
transverse momentum and longitudinal momentum fraction are
reported for seven bins in collision centrality for R=0.4
jets with pTjet>100 GeV. Commensurate minimum pT values are
used for the other radii. Ratios of fragment distributions
in each centrality bin to those measured in the most
peripheral bin are presented. These ratios show a reduction
of fragment yield in central collisions relative to
peripheral collisions at intermediate z values,
0.04≲z≲0.2, and an enhancement in fragment yield for
z≲0.04. A smaller, less significant enhancement is
observed at large z and large pT in central
collisions.},
Doi = {10.1016/j.physletb.2014.10.065},
Key = {fds314175}
}
@article{fds321312,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of indirect CP -violating asymmetries in D0
→k+K- and D0 →π+π- decays at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.90.111103},
Abstract = {We report a measurement of the indirect CP-violating
asymmetries (AΓ) between effective lifetimes of anticharm
and charm mesons reconstructed in D0→K+K- and D0→π+π-
decays. We use the full data set of proton-antiproton
collisions collected by the Collider Detector at Fermilab
experiment and corresponding to 9.7fb-1 of integrated
luminosity. The strong-interaction decay D∗+→D0π+ is
used to identify the meson at production as D0 or D¯0. We
statistically subtract D0 and D¯0 mesons originating from
b-hadron decays and measure the yield asymmetry between
anticharm and charm decays as a function of decay time. We
measure AΓ(K+K-)=(-0.19±0.15(stat)±0.04(syst))% and
AΓ(π+π-)=(-0.01±0.18(stat)±0.03(syst))%. The results
are consistent with the hypothesis of CP symmetry and their
combination yields AΓ=(-0.12±0.12)%.},
Doi = {10.1103/PhysRevD.90.111103},
Key = {fds321312}
}
@article{fds308360,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Measurement of isolated-photon pair production in pp
collisions at √s=7TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {1},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2013)086},
Abstract = {The ATLAS experiment at the LHC has measured the production
cross section of events with two isolated photons in the
final state, in proton-proton collisions at √s=7TeV . The
full data set collected in 2011, corresponding to an
integrated luminosity of 4.9 fb-1, is used. The amount of
background, from hadronic jets and isolated electrons, is
estimated with data-driven techniques and subtracted. The
total cross section, for two isolated photons with
transverse energies above 25 GeV and 22 GeV respectively, in
the acceptance of the electromagnetic calorimeter (|η| <
1.37 and 1.52 < |η| < 2.37) and with an angular separation
ΔR > 0.4, is 44.0-4.2+3.2 pb. The differential cross
sections as a function of the di-photon invariant mass,
transverse momentum, azimuthal separation, and cosine of the
polar angle of the largest transverse energy photon in the
Collins-Soper di-photon rest frame are also measured. The
results are compared to the prediction of leading-order
parton-shower and next-to-leading-order and
next-to-next-to-leading-order parton-level
generators.[Figure not available: see fulltext.] © 2013
CERN for the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP01(2013)086},
Key = {fds308360}
}
@article{fds308792,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbara, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonusnkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Brink,
SVD and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and Dejongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr,
EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furie, I and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold, M and Goldstein,
J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Guo, RS and Haas, RM and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara,
K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Herndon, M and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kirby, M and Kirk, M and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu,
YC and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi,
N and Moore, E and Moore, R and Morita, Y and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman,
J and Nahn, S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pappas, SP and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos, F and Pukhov, O and Punzi, G and Ragan, K and Rakitine, A and Reher, D and Reichold, A and Riegler, W and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson,
A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Safonov, A and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi,
L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt,
MP and Schmitt, M and Scodellaro, E and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo,
P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka,
M and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi,
K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa, F and Vaiciulis, T and Valls, J and III, SV and Velev, G and Vidal, R and Vilar,
R and Volobouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl,
J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and III,
WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh,
GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu,
Z and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of J / ψ and ψ (2S) polarization in pp̄
collisions at √s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {85},
Number = {14},
Pages = {2886-2891},
Year = {2000},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.85.2886},
Abstract = {We have measured the polarization of J/ψ and ψ(2S) mesons
produced in pp̄ collisions at √s = 1.8 TeV, using data
collected at the Collider Detector at Fermilab during
1992-1995. The polarization of promptly produced J/ψ
[ψ(2S)] mesons is isolated from those produced in B-hadron
decay, and measured over the kinematic range 4 [5.5] < PT
< 20 GeV/c and |y| < 0.6. For PT ≳ 12 GeV/c we do
not observe significant polarization in the prompt
component. © 2000 The American Physical
Society.},
Doi = {10.1103/physrevlett.85.2886},
Key = {fds308792}
}
@article{fds321167,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Measurement of jet activity in top quark events using the
eμ final state with two b-tagged jets in pp collisions at
√s=8 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {9},
Publisher = {Springer Nature},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2016)074},
Abstract = {Measurements of the jet activity in tt¯ events produced in
proton-proton collisions at s=8 TeV are presented, using
20.3 fb−1 of data collected by the ATLAS experiment at the
Large Hadron Collider. The events were selected in the
dilepton eμ decay channel with two identified b-jets. The
numbers of additional jets for various jet transverse
momentum (pT) thresholds, and the normalised differential
cross-sections as a function of pT for the five highest-pT
additional jets, were measured in the jet pseudo-rapidity
range |η| < 4.5. The gap fraction, the fraction of events
which do not contain an additional jet in a central rapidity
region, was measured for several rapidity intervals as a
function of the minimum pT of a single jet or the scalar sum
of pT of all additional jets. These fractions were also
measured in different intervals of the invariant mass of the
eμbb¯ system. All measurements were corrected for detector
effects, and found to be mostly well-described by
predictions from next-to-leading-order and leading-order
tt¯ event generators with appropriate parameter choices.
The results can be used to further optimise the parameters
used in such generators.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP09(2016)074},
Key = {fds321167}
}
@article{fds308357,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat,
P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiarella,
V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
RN},
Title = {Measurement of jet shapes in top-quark pair events at
[Formula: see text] using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {12},
Pages = {2676},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2676-3},
Abstract = {A measurement of jet shapes in top-quark pair events using
1.8 fb<sup>-1</sup> of [Formula: see text]<i>pp</i>
collision data recorded by the ATLAS detector at the LHC is
presented. Samples of top-quark pair events are selected in
both the single-lepton and dilepton final states. The
differential and integrated shapes of the jets initiated by
bottom-quarks from the top-quark decays are compared with
those of the jets originated by light-quarks from the
hadronic <i>W</i>-boson decays [Formula: see text] in the
single-lepton channel. The light-quark jets are found to
have a narrower distribution of the momentum flow inside the
jet area than <i>b</i>-quark jets.},
Doi = {10.1140/epjc/s10052-013-2676-3},
Key = {fds308357}
}
@article{fds365410,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Measurement of light-by-light scattering and search for
axion-like particles with 2.2 nb−1 of Pb+Pb
data with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {3},
Year = {2021},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2021)243},
Abstract = {This paper describes a measurement of light-by-light
scattering based on Pb+Pb collision data recorded by the
ATLAS experiment during Run 2 of the LHC. The study uses 2.2
nb−1 of integrated luminosity collected in 2015 and 2018
at sNN = 5.02 TeV. Light-by-light scattering candidates are
selected in events with two photons produced exclusively,
each with transverse energy ETγ> 2.5 GeV, pseudorapidity
|ηγ| < 2.37, diphoton invariant mass mγγ> 5 GeV, and
with small diphoton transverse momentum and diphoton
acoplanarity. The integrated and differential fiducial cross
sections are measured and compared with theoretical
predictions. The diphoton invariant mass distribution is
used to set limits on the production of axion-like
particles. This result provides the most stringent limits to
date on axion-like particle production for masses in the
range 6–100 GeV. Cross sections above 2 to 70 nb are
excluded at the 95% CL in that mass interval. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP03(2021)243},
Key = {fds365410}
}
@article{fds321324,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurement of long-range pseudorapidity correlations and
azimuthal harmonics in √sNN =5.02 TeV
proton-lead collisions with the ATLAS detector},
Journal = {Physical Review C - Nuclear Physics},
Volume = {90},
Number = {4},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevC.90.044906},
Abstract = {Measurements of two-particle correlation functions and the
first five azimuthal harmonics, v1 to v5, are presented,
using 28 nb-1 of p+Pb collisions at a nucleon-nucleon
center-of-mass energy of √sNN=5.02 TeV measured with the
ATLAS detector at the LHC. Significant long-range
"ridgelike" correlations are observed for pairs with small
(|Δϕ|<π/3) and back-to-back pairs (|Δφ|>2π/3) over the
transverse momentum range 0.4<pT<12 GeV and in different
intervals of event activity. The event activity is defined
by either the number of reconstructed tracks or the total
transverse energy on the Pb-fragmentation side. The
azimuthal structure of such long-range correlations is
Fourier decomposed to obtain the harmonics νn as a function
of pT and event activity. The extracted νn values for n=2
to 5 decrease with n. The ν2 and ν3 values are found to be
positive in the measured pT range. The ν1 is also measured
as a function of pT and is observed to change sign around
pT≈1.5-2.0 GeV and then increase to about 0.1 for pT>4
GeV. The ν2 (pT), ν3 (pT), and ν4 (pT) are compared to
the νn coefficients in Pb+Pb collisions at √sNN=2.76 TeV
with similar event multiplicities. Reasonable agreement is
observed after accounting for the difference in the average
pT of particles produced in the two collision
systems.},
Doi = {10.1103/PhysRevC.90.044906},
Key = {fds321324}
}
@article{fds308677,
Author = {Abulencia, and A, and others},
Title = {Measurement of mass and width of the excited charmed meson
states D10 and D2*0},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {5},
Pages = {051104},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.73.051104},
Abstract = {We report on precision measurements of the masses and widths
of the narrow, orbitally excited states D0_1 and D*0_2 using
the CDF II detector at the Fermilab Tevatron. Both states
(collectively called D**) are reconstructed in the decay
channel D** --> D*+ pi+-. The D*0_s is also reconstructed in
the D** --> D+ pi+- channel. Using a dataset with an
integrated luminosity of 210 pb-1, the measured masses and
widths for the D0_1 are 2421.7 +/- 0.7 +/- 0.6 MeV/c2 and
20.0 +/- 1.7 +/- 1.3 MeV/c2 respectively, while for the
D*0_2 they are 2463.3 +/- 0.6 +/- 0.8 MeV/c2 and 49.2 +/-
2.3 +/- 1.2 MeV/c2. These values are currently the single
best measurements available.},
Doi = {10.1103/PhysRevD.73.051104},
Key = {fds308677}
}
@article{fds375955,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA},
Title = {Measurement of muon pairs produced via γγ scattering in
nonultraperipheral Pb + Pb collisions at √sNN = 5.02 TeV
with the ATLAS detector},
Journal = {Physical Review C},
Volume = {107},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevC.107.054907},
Abstract = {Results of a measurement of dimuon photoproduction in
nonultraperipheral Pb + Pb collisions at √sNN = 5.02 TeV
are presented. Themeasurement uses ATLAS data from the 2015
and 2018 Pb + Pb data-taking periods at the LHC with an
integrated luminosity of 1.94 nb.1. The γγ → μ+ μ-
pairs are identified via selections on pair momentum
asymmetry and acoplanarity. Differential cross sections for
dimuon production are measured in different centrality,
average muon momentum, and pair rapidity intervals as
functions of acoplanarity and k⊥, the transverse momentum
kick of one muon relative to the other. Measurements are
also made as a function of the rapidity separation of the
muons and the angle of the muon pair relative to the
second-order event plane to test whether magnetic fields
generated in the quark-gluon plasma affect the measured
muons. A prior observation of a centrality-dependent
broadening of the acoplanarity distribution is confirmed.
Furthermore, the improved precision of the measurement
reveals a depletion in the number of pairs having small
acoplanarity or k⊥ values in more central collisions. The
acoplanarity distributions in a given centrality interval
are observed to vary with the mean pT of the muons in the
pair, but the k⊥ distributions do not. Comparisons with
recent theoretical predictions are made. The predicted
trends associated with effects of magnetic fields on the
dimuons are not observed.},
Doi = {10.1103/PhysRevC.107.054907},
Key = {fds375955}
}
@article{fds308722,
Author = {Acosta, D and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli, M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri,
A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, J and Frisch,
H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu,
T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic,
P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin,
A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa,
T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patricck, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio,
S and Ratnikov, F and Ray, H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna,
G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar,
S and Sato, K and Savard, P and Savoy-Navarro, A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet,
M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smirnov, D and Smith, JR and Snider,
FD},
Title = {Measurement of partial widths and search for direct CP
violation in D 0 meson decays to
K-K+ and π -π+},
Journal = {Physical Review Letters},
Volume = {94},
Number = {12},
Pages = {122001},
Year = {2005},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.94.122001},
Abstract = {We present a measurement of relative partial widths and
decay rate CP asymmetries in K- K+ and π-π+ decays of D0
mesons produced in pp̄ collisions at,√s = 1.96 TeV. We
use a sample of 2 × 105 D*+ →D0π+ (and charge conjugate)
decays with the D0 decaying to K-π+, K-K +, and π-π+,
corresponding to 123 pb -1 of data collected by the Collider
Detector at Fermilab II experiment at the Fermilab Tevatron
collider. No significant direct CP violation is observed. We
measure γ(D0→ K- K +)/γ(D0-→K-π+) = 0.0992 ±0.0992
±0.0012, γ(D0→K -π+)/γ(D0→K -π+) = 0.03594 ±
0.00054 ±0.00040, A CP(K- K+) = (2.0 ±1.2 ±0.6)%, and
ACP(π-π+) = (1.0 ±1.3 ±0.6)%, where, in all cases, the
first uncertainty is statistical and the second is
systematic. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.94.122001},
Key = {fds308722}
}
@article{fds308565,
Author = {Aaltonen, T and others},
Title = {Measurement of particle production and inclusive
differential cross sections in pp̅ collisions at sqrt[s]
=1.96 TeV},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {11},
Pages = {112005},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.112005},
Abstract = {We report a set of measurements of particle production in
inelastic pp̅ collisions collected with a minimum-bias
trigger at the Tevatron Collider with the CDF II experiment.
The inclusive charged particle transverse momentum
differential cross section is measured, with improved
precision, over a range about ten times wider than in
previous measurements. The former modeling of the spectrum
appears to be incompatible with the high particle momenta
observed. The dependence of the charged particle transverse
momentum on the event particle multiplicity is analyzed to
study the various components of hadron interactions. This is
one of the observable variables most poorly reproduced by
the available Monte Carlo generators. A first measurement of
the event transverse energy sum differential cross section
is also reported. A comparison with a pythia prediction at
the hadron level is performed. The inclusive
charged-particle differential production cross section is
fairly well reproduced only in the transverse momentum range
available from previous measurements. At higher momentum the
agreement is poor. The transverse energy sum is poorly
reproduced over the whole spectrum. The dependence of the
charged particle transverse momentum on the particle
multiplicity needs the introduction of more sophisticated
particle production mechanisms, such as multiple parton
interactions, in order to be better explained.},
Doi = {10.1103/PhysRevD.79.112005},
Key = {fds308565}
}
@article{fds308424,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rosner, JL and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester,
WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang,
YC},
Title = {Measurement of polarization and search for CP violation in
B(s)0→φφ decays.},
Journal = {Physical review letters},
Volume = {107},
Number = {26},
Pages = {261802},
Year = {2011},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.107.261802},
Abstract = {We present the first measurement of polarization and
CP-violating asymmetries in a B(s)(0) decay into two light
vector mesons, B(s)(0)→φφ, and an improved determination
of its branching ratio using 295 decays reconstructed in a
data sample corresponding to 2.9 fb(-1) of integrated
luminosity collected by the CDF experiment at the Fermilab
Tevatron collider. The fraction of longitudinal polarization
is determined to be f(L)=0.348±0.041(stat)±0.021(syst),
and the branching ratio B(B(s)(0)→φφ)=[2.32±0.18(stat)±0.82(syst)]×10(-5).
Asymmetries of decay angle distributions sensitive to CP
violation are measured to be A(u)=-0.007±0.064(stat)±0.018(syst)
and A(v)=-0.120±0.064(stat)±0.016(syst).},
Doi = {10.1103/physrevlett.107.261802},
Key = {fds308424}
}
@article{fds308747,
Author = {Collaboration, DAEACDFII},
Title = {Measurement of Prompt Charm Meson Production Cross Sections
in pp-bar Collisions at sqrt[s]=1.96 TeV},
Journal = {Physical Review Letters},
Volume = {91},
Number = {24},
Pages = {241804},
Year = {2003},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.91.241804},
Abstract = {We report on measurements of differential cross sections d
sigma /dpT for prompt charm meson production in pp-bar
collisions at sqrt[s]=1.96 TeV using 5.8±0.3 pb-1 of data
from the CDF II detector at the Fermilab Tevatron. The data
are collected with a new trigger that is sensitive to the
long lifetime of hadrons containing heavy flavor. The charm
meson cross sections are measured in the central rapidity
region |y| K- pi +, D*+-->D0 pi +, D+-->K- pi + pi +, D+s-->
phi pi +, and their charge conjugates. The measured cross
sections are compared to theoretical calculations.},
Doi = {10.1103/physrevlett.91.241804},
Key = {fds308747}
}
@article{fds311120,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Measurement of R=B(t→Wb)/B(t→Wq) in top-quark-pair
decays using lepton+jets events and the full CDF run II
dataset},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.87.111101},
Abstract = {We present a measurement of the ratio of the top-quark
branching fractions R=B(t→Wb)/B(t→Wq), where q
represents quarks of type b, s, or d, in the final state
with a lepton and hadronic jets. The measurement uses
√s=1.96 TeV proton-antiproton collision data from 8.7 fb-1
of integrated luminosity collected with the Collider
Detector at Fermilab during Run II of the Tevatron. We
simultaneously measure R=0.94±0.09 (stat+syst) and the tt̄
production cross section σtt̄=7. 5±1.0 (stat+syst) pb.
The magnitude of the Cabibbo-Kobayashi-Maskawa matrix
element, |Vtb|=0.97±0.05 (stat+syst) is extracted assuming
three generations of quarks, and a lower limit of |V
tb|>0.89 at 95% credibility level is set. © 2013 American
Physical Society.},
Doi = {10.1103/PhysRevD.87.111101},
Key = {fds311120}
}
@article{fds308531,
Author = {Aaltonen, T and others},
Title = {Measurement of Resonance Parameters of Orbitally Excited
Narrow B[sup 0] Mesons},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {10},
Pages = {102003},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.102003},
Abstract = {We report a measurement of resonance parameters of the
orbitally excited (L=1) narrow B0 mesons in decays to
B;{(*)+}pi;{-} using 1.7 fb;{-1} of data collected by the
CDF II detector at the Fermilab Tevatron. The mass and width
of the B_{2};{*0} state are measured to be
m(B_{2};{*0})=5740.2_{-1.8};{+1.7}(stat)-0.8+0.9(syst)
MeV/c;{2} and Gamma(B_{2};{*0})=22.7_{-3.2};{+3.8}(stat)-10.2+3.2(syst)
MeV/c;{2}. The mass difference between the B_{2};{*0} and
B10 states is measured to be 14.9_{-2.5};{+2.2}(stat)-1.4+1.2(syst)
MeV/c;{2}, resulting in a B10 mass of 5725.3_{-2.2};{+1.6}(stat)-1.5+1.4(syst)
MeV/c;{2}. This is currently the most precise measurement of
the masses of these states and the first measurement of the
B_{2};{*0} width.},
Doi = {10.1103/physrevlett.102.102003},
Key = {fds308531}
}
@article{fds308651,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Casarsa, M and Castro,
A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Cyr,
D and DaRonco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De
Lentdecker, G and Dell'Orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni,
GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and DiTuro, P and Dörr,
C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell,
JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Guimaraes da
Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Le, Y and LeCompte, T and Lee, J and Lee,
YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister,
A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean,
R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Movilla
Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ranjan,
N and Rappoccio, S and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin, J},
Title = {Measurement of sigma Lambda b0/sigma B0 x B(Lambda
b0-->Lambda c+pi-)/B(B0-->D+pi-) in pp collisions at square
root s=1.96 TeV.},
Journal = {Physical review letters},
Volume = {98},
Number = {12},
Pages = {122002},
Year = {2007},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.98.122002},
Abstract = {We present the first observation of the baryon decay Lambda
b0-->Lambda c+pi- followed by Lambda c+-->pK-pi+ in 106 pb-1
pp collisions at square root s=1.96 TeV in the CDF
experiment. In order to reduce systematic error, the
measured rate for Lambda b0 decay is normalized to the
kinematically similar meson decay B0-->D+pi- followed by
D+-->pi+K-pi+. We report the ratio of production cross
sections (sigma) times the ratio of branching fractions (B)
for the momentum region integrated above pT>6 GeV/c and
pseudorapidity range |eta|<1.3: sigma(pp-->Lambda
b0X)/sigma(pp-->B0X)xB(Lambda b0-->Lambda
c+pi-)/B(B0-->D+pi-)=0.82+/-0.08(stat)+/-0.11(syst)+/-0.22[B(Lambda
c+-->pK-pi+)].},
Doi = {10.1103/physrevlett.98.122002},
Key = {fds308651}
}
@article{fds308803,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Antos, J and Apollinari, G and Arisawa,
T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge,
JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker,
C and Bloom, K and Blumenfeld, B and Blusk, BS and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and Brink, SVD and Bromberg, C and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto,
G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Cobal, M and Cocca, E and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Costa, JGD and Costanzo, D and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
RG and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold, M and Goldstein,
J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser,
J and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck,
C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara,
H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov,
A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and Lee,
AM and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Meschi, E and Mesropian, C and Miao, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Moggi, N and Moore, E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman,
J and Nahn, S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pappas, SP and Parri, A and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom,
L and Pope, G and Prokoshin, F and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson,
L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni,
A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano,
A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo,
P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki,
T and Takashima, R and Takikawa, K and Tanaka, M and Takano, T and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk,
S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Ukegawa, F and Valls, J and Vejcik, S and Velev, G and Vidal, R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of sin 2β from B→J/φKs0
with the CDF detector},
Journal = {Physical Review D},
Volume = {61},
Number = {7},
Pages = {1-16},
Year = {2000},
Abstract = {This paper reports an updated measurement of the standard
model CP violation parameter sin 2β using the CDF Detector
at Fermilab. The entire run I data sample of 110 pb-1 of
proton-antiproton collisions at √s = 1.8 TeV is used to
identify a signal sample of ∼400 B→J/φKs0 events, where
J/φ→μ+μ- →μ+μ-. The flavor of the neutral B meson
is identified at the time of production by combining
information from three tagging algorithms: a same-side tag,
a jet-charge tag, and a soft-lepton tag. A maximum
likelihood fitting method is used to determine sin
2β=0.79-0.44+0.41(stat+syst). This value of sin 2β is
consistent with the standard model prediction, based upon
existing measurements, of a large positive CP-violating
asymmetry in this decay mode. ©2000 The American Physical
Society.},
Key = {fds308803}
}
@article{fds308804,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Antos, J and Apollinari, G and Arisawa,
T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge,
JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker,
C and Bloom, K and Blumenfeld, B and Blusk, BS and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and Brink, SVD and Bromberg, C and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto,
G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Cobal, M and Cocca, E and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Costa, JGD and Costanzo, D and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and Dejongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr,
EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold, M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Guo,
RS and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara,
H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov,
A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and IV,
AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Meschi, E and Mesropian, C and Miao, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Moggi, N and Moore, E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman,
J and Nahn, S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pappas, SP and Parri, A and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom,
L and Pope, G and Prokoshin, F and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson,
L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni,
A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano,
A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo,
P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki,
T and Takashima, R and Takikawa, K and Tanaka, M and Takano, T and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk,
S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Ukegawa, F and Valls, J and III, SV and Velev, G and Vidal, R and Vilar, R and Vologouev,
I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Watts,
T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu,
I and Yu, S and Zanetti, A and Zetti, F and Zucchelli,
S},
Title = {Measurement of sin2β from B→J/ψKS0
with the CDF detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {61},
Number = {7},
Pages = {1-16},
Year = {2000},
Abstract = {This paper reports an updated measurement of the standard
model CP violation parameter sin 2β using the CDF Detector
at Fermilab. The entire run I data sample of 110 pb-1 of
proton-antiproton collisions at √s =1.8 TeV is used to
identify a signal sample of ∼400 B→J/ψKS0 events, where
J/ψ→μ+μ- and KS0 →π+π-. The flavor of the neutral B
meson is identified at the time of production by combining
information from three tagging algorithms: a same-side tag,
a jet-charge tag, and a soft-lepton tag. A maximum
likelihood fitting method is used to determine
sin2β=0.19-0.44+0.41(stat+syst). This value of sin 2β is
consistent with the standard model prediction, based upon
existing measurements, of a large positive CP-violating
asymmetry in this decay mode. ©2000 The American Physical
Society.},
Key = {fds308804}
}
@article{fds321193,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Erbacher, R and Errede, S and Esham,
B},
Title = {Measurement of sin2 θefflept
using e+e- pairs from γ∗/Z bosons produced in
pp collisions at a center-of-momentum energy of 1.96
TeV},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112016},
Abstract = {At the Fermilab Tevatron proton-antiproton (pp) collider,
Drell-Yan lepton pairs are produced in the process
pp→e+e-+X through an intermediate γ∗/Z boson. The
forward-backward asymmetry in the polar-angle distribution
of the e- as a function of the e+e - pair mass is used to
obtain sin2θefflept, the effective leptonic determination
of the electroweak-mixing parameter sin2θW. The measurement
sample, recorded by the Collider Detector at Fermilab (CDF),
corresponds to 9.4 fb-1 of integrated luminosity from pp
collisions at a center-of-momentum energy of 1.96 TeV, and
is the full CDF Run II data set. The value of sin2θefflept
is found to be 0.23248±0.00053. The combination with the
previous CDF measurement based on μ+μ- pairs yields
sin2θefflept=0.23221±0.00046. This result, when
interpreted within the specified context of the standard
model assuming sin2θW=1-MW2/MZ2 and that the W- and Z-boson
masses are on-shell, yields sin2θW=0.22400±0.00045, or
equivalently a W-boson mass of 80.328±0.024
GeV/c2.},
Doi = {10.1103/PhysRevD.93.112016},
Key = {fds321193}
}
@article{fds365379,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Bella, LA and Arabidze, G},
Title = {Measurement of single top-quark production in association
with a W boson in the single-lepton channel at √s=8TeV
with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {8},
Year = {2021},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09371-7},
Abstract = {The production cross-section of a top quark in association
with a W boson is measured using proton–proton collisions
at s=8TeV. The dataset corresponds to an integrated
luminosity of 20.2fb-1, and was collected in 2012 by the
ATLAS detector at the Large Hadron Collider at CERN. The
analysis is performed in the single-lepton channel. Events
are selected by requiring one isolated lepton (electron or
muon) and at least three jets. A neural network is trained
to separate the tW signal from the dominant tt¯ background.
The cross-section is extracted from a binned profile
maximum-likelihood fit to a two-dimensional discriminant
built from the neural-network output and the invariant mass
of the hadronically decaying W boson. The measured
cross-section is σtW=26±7pb, in good agreement with the
Standard Model expectation.},
Doi = {10.1140/epjc/s10052-021-09371-7},
Key = {fds365379}
}
@article{fds321258,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli,
F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak,
L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi,
M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov,
AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T},
Title = {Measurement of spin correlation in top-antitop quark events
and search for top squark pair production in pp collisions
at √s=8 TeV using the ATLAS detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {14},
Pages = {142001},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.114.142001},
Abstract = {A measurement of spin correlation in tt[over ¯] production
is presented using data collected with the ATLAS detector at
the Large Hadron Collider in proton-proton collisions at a
center-of-mass energy of 8 TeV, corresponding to an
integrated luminosity of 20.3 fb^{-1}. The correlation
between the top and antitop quark spins is extracted from
dilepton tt[over ¯] events by using the difference in the
azimuthal angle between the two charged leptons in the
laboratory frame. In the helicity basis the measured degree
of correlation corresponds to A_{helicity}=0.38±0.04, in
agreement with the standard model prediction. A search is
performed for pair production of top squarks with masses
close to the top quark mass decaying to predominantly
right-handed top quarks and a light neutralino, the lightest
supersymmetric particle. Top squarks with masses between the
top quark mass and 191 GeV are excluded at the 95%
confidence level.},
Doi = {10.1103/physrevlett.114.142001},
Key = {fds321258}
}
@article{fds375952,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
M and Bouquet, R and Marchiori, G and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
Gemmeren, P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Cui,
Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Unal, M and Webb, AF and Huseynov, N and Ahmadov, F and Agaras, MN and Bosman,
M},
Title = {Measurement of substructure-dependent jet suppression in
Pb+Pb collisions at 5.02 TeV with the ATLAS
detector},
Journal = {Physical Review C},
Volume = {107},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevC.107.054909},
Abstract = {The ATLAS detector at the Large Hadron Collider has been
used to measure jet substructure modification and
suppression in Pb+Pb collisions at a nucleon–nucleon
center-of-mass energy √sNN = 5.02 TeV in comparison with
proton–proton (pp) collisions at √s = 5.02 TeV. The
Pb+Pb data, collected in 2018, have an integrated luminosity
of 1.72 nb−1, while the ppdata, collected in 2017, have an
integrated luminosity of 260 pb−1. Jets used in this
analysis are clustered using the anti-kt algorithm with a
radius parameter R = 0.4. The jet constituents, defined by
both tracking and calorimeter information, are used to
determine the angular scale rg of the first hard splitting
inside the jet by reclustering them using the
Cambridge–Aachen algorithm and employing the soft-drop
grooming technique. The nuclear modification factor, RAA,
used to characterize jet suppression in Pb+Pb collisions, is
presented differentially in rg, jet transverse momentum, and
in intervals of collision centrality. The RAA value is
observed to depend significantly on jet rg. Jets produced
with the largest measured rg are found to be twice as
suppressed as those with the smallest rg in central Pb+Pb
collisions. The RAA values do not exhibit a strong variation
with jet pT in any of the rg intervals. The rg and pT
dependence of jet RAA is qualitatively consistent with a
picture of jet quenching arising from coherence and provides
the most direct evidence in support of this
approach.},
Doi = {10.1103/PhysRevC.107.054909},
Key = {fds375952}
}
@article{fds375905,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai,
K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos,
R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron
Moreno, DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga,
D and Bauce, M and Bauer, P and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli,
M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya,
DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul,
A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman,
M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger,
D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruncko,
D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson,
BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter,
JWS and Carter, TM and Casado, MP and Casha, AF and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen,
A and Chen, B and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ and Clavijo
Columbie, JM and Clawson, SE and Clement, C and Clercx, J and Clissa, L and Coadou, Y and Cobal, M and Coccaro, A and Barrue, RFC and Coelho Lopes
De Sa and R},
Title = {Measurement of Suppression of Large-Radius Jets and Its
Dependence on Substructure in Pb+Pb Collisions at
sqrt[s_{NN}]=5.02 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {17},
Pages = {172301},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.131.172301},
Abstract = {This letter presents a measurement of the nuclear
modification factor of large-radius jets in
sqrt[s_{NN}]=5.02 TeV Pb+Pb collisions by the ATLAS
experiment. The measurement is performed using
1.72 nb^{-1} and 257 pb^{-1} of Pb+Pb and pp data,
respectively. The large-radius jets are reconstructed with
the anti-k_{t} algorithm using a radius parameter of R=1.0,
by reclustering anti-k_{t} R=0.2 jets, and are measured over
the transverse momentum (p_{T}) kinematic range of
158<p_{T}<1000 GeV and absolute pseudorapidity |y|<2.0.
The large-radius jet constituents are further reclustered
using the k_{t} algorithm in order to obtain the splitting
parameters, sqrt[d_{12}] and ΔR_{12}, which characterize
the transverse momentum scale and angular separation for the
hardest splitting in the jet, respectively. The nuclear
modification factor, R_{AA}, obtained by comparing the Pb+Pb
jet yields to those in pp collisions, is measured as a
function of jet transverse momentum (p_{T}) and sqrt[d_{12}]
or ΔR_{12}. A significant difference in the quenching of
large-radius jets having single subjet and those with more
complex substructure is observed. Systematic comparison of
jet suppression in terms of R_{AA} for different jet
definitions is also provided. Presented results support the
hypothesis that jets with hard internal splittings lose more
energy through quenching and provide a new perspective for
understanding the role of jet structure in jet
suppression.},
Doi = {10.1103/physrevlett.131.172301},
Key = {fds375905}
}
@article{fds308639,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $p \bar{p} \to t \bar{t}$ production
cross- section and the top quark mass at $\sqrt{s}$ = 1.96-
TeV in the all-hadronic decay mode},
Journal = {Phys. Rev.},
Volume = {D76},
Number = {7},
Pages = {072009},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.76.072009},
Abstract = {We report the measurements of the t[overline t] production
cross section and of the top quark mass using 1.02 fb-1 of
p[overline p] data collected with the CDF II detector at the
Fermilab Tevatron. We select events with six or more jets on
which a number of kinematical requirements are imposed by
means of a neural network algorithm. At least one of these
jets must be identified as initiated by a b-quark candidate
by the reconstruction of a secondary vertex. The cross
section is measured to be sigmat[overline
t]=8.3$\pm$1.0(stat)-1.5+2.0(syst)$\pm$0.5(lumi) pb, which
is consistent with the standard model prediction. The top
quark mass of 174.0$\pm$2.2(stat)$\pm$4.8(syst) GeV/c2 is
derived from a likelihood fit incorporating reconstructed
mass distributions representative of signal and
background.},
Doi = {10.1103/PhysRevD.76.072009},
Key = {fds308639}
}
@article{fds308489,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $t \bar{t}$ Production Cross Section in
$p \bar{p}$ Collisions at $\sqrt{s} = 1.96$ TeV using Soft
Electron $b$-Tagging},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {9},
Pages = {092002},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.092002},
Abstract = {http://arxiv.org/abs/1002.3783},
Doi = {10.1103/PhysRevD.81.092002},
Key = {fds308489}
}
@article{fds308776,
Author = {collaboration, CDF},
Title = {Measurement of the $t\bar{t}$ Production Cross Section in
$p\bar{p}$ Collisions at $\sqrt{s}=1.8 TeV$},
Journal = {Phys. Rev.},
Volume = {D64},
Number = {032002},
Publisher = {Springer Nature},
Year = {2001},
Month = {January},
url = {http://arXiv.org/ps/hep-ex/0101036},
Abstract = {http://arXiv.org/ps/hep-ex/0101036},
Doi = {10.1007/JHEP04(2012)093},
Key = {fds308776}
}
@article{fds308664,
Author = {Abulencia, and A, and others},
Title = {Measurement of the $t\bar{t}$ production cross section in
$p\bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV using missing
$E_t$ + jets events with secondary vertex $b-
$tagging},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {20},
Pages = {202002},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.202002},
Abstract = {We present a measurement of the tt-bar production cross
section in p anti-p collisions at s**(1/2) = 1.96 TeV which
uses events with an inclusive signature of significant
missing transverse energy and jets. This is the first
measurement which makes no explicit lepton identification
requirements, so that sensitivity to W --> tau nu decays is
maintained. Heavy flavor jets from top quark decay are
identified with a secondary vertex tagging algorithm. From
311 pb-1 of data collected by the Collider Detector at
Fermilab we measure a production cross section of 5.8 +/-
1.2(stat.)+0.9_-0.7(syst.) pb for a top quark mass of 178
GeV/c2, in agreement with previous determinations and
standard model predictions.},
Doi = {10.1103/physrevlett.96.202002},
Key = {fds308664}
}
@article{fds308455,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of the $t\overline{t}$ production cross section
in $p\overline{p}$ collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$
using events with large missing transverse energy and
jets},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {3},
Pages = {032003},
Publisher = {American Physical Society},
Year = {2011},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.84.032003},
Abstract = {In this paper we report a measurement of the tt̄ production
cross section in pp̄ collisions at √s=1.96TeV using data
corresponding to an integrated luminosity of 2.2fb-1
collected with the CDF II detector at the Tevatron
accelerator. We select events with significant missing
transverse energy and high jet multiplicity. This
measurement vetoes the presence of explicitly identified
electrons and muons, thus enhancing the tau contribution of
tt̄ decays. Signal events are discriminated from the
background using a neural network, and heavy flavor jets are
identified by a secondary-vertex tagging algorithm. We
measure a tt̄ production cross section of
7.99±0.55(stat)±0.76(syst)±0.46(lumi) pb, assuming a top
mass mtop=172.5GeV/c2, in agreement with previous
measurements and standard model predictions. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.84.032003},
Key = {fds308455}
}
@article{fds308450,
Author = {Aaltonen, and and, T and al, E},
Title = {Measurement of the $t\overline{t}$ production cross section
with an \textit{in~situ} calibration of $b$-jet
identification efficiency},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {7},
Pages = {071102},
Publisher = {American Physical Society},
Year = {2011},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.83.071102},
Abstract = {A measurement of the top-quark pair-production cross section
in pp̄ collisions at √s=1.96TeV using data corresponding
to an integrated luminosity of 1.12fb-1 collected with the
Collider Detector at Fermilab is presented. Decays of
top-quark pairs into the final states eν+ jets and μν+
jets are selected, and the cross section and the b-jet
identification efficiency are determined using a new
measurement technique which requires agreement between the
measured cross sections with exactly one and with multiple
identified b quarks from the top-quark decays. Assuming a
top-quark mass of 175GeV/c2, a cross section of
8.5±0.6(stat)±0. 7(syst)pb is measured. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevD.83.071102},
Key = {fds308450}
}
@article{fds308509,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $WW+WZ$ production cross section using a
matrix element technique in $lepton+jets$
events},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {11},
Pages = {112001},
Publisher = {American Physical Society},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.82.112001},
Abstract = {We present a measurement of the WW+WZ production cross
section observed in a final state consisting of an
identified electron or muon, two jets, and missing
transverse energy. The measurement is carried out in a data
sample corresponding to up to 4.6fb⊃-1 of integrated
luminosity at √s=1.96TeV collected by the CDF II detector.
Matrix element calculations are used to separate the diboson
signal from the large backgrounds. The WW+WZ cross section
is measured to be 17.4±3.3pb in agreement with standard
model predictions. A fit to the dijet invariant mass
spectrum yields a compatible cross section measurement. ©
2010 The American Physical Society.},
Doi = {10.1103/PhysRevD.82.112001},
Key = {fds308509}
}
@article{fds308483,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $WW+WZ$ Production Cross Section Using
the Lepton+Jets Final State at CDF II},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {10},
Pages = {101801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.101801},
Abstract = {http://arxiv.org/abs/0911.4449},
Doi = {10.1103/PhysRevLett.104.101801},
Key = {fds308483}
}
@article{fds43834,
Author = {S. Cabrera and S. Carron and A. Goshaw and Y. Huang and M. Kruse (Duke
U.) and D. Acosta et al. (CDF Collaboration)},
Title = {Measurement of the $W^+ W^-$ Production Cross Section in
$p\bar{p}$ Collisions at $\sqrt{s} = 1.96$ TeV Using
Dilepton Events},
Journal = {Phys. Rev. Lett.},
Volume = {94},
Number = {211801},
Year = {2005},
url = {http://arxiv.org/pdf/hep-ex/0501050},
Abstract = {http://arxiv.org/abs/hep-ex/0501050},
Key = {fds43834}
}
@article{fds308478,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $W^+W^-$ Production Cross Section and
Search for Anomalous $WW\gamma$ and $WWZ$ Couplings in $p
\bar p$ Collisions at $\sqrt{s} = 1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {20},
Pages = {201801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.201801},
Abstract = {http://arxiv.org/abs/0912.4500},
Doi = {10.1103/PhysRevLett.104.201801},
Key = {fds308478}
}
@article{fds308482,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $\Lambda_b$ Lifetime in $\Lambda_b \to
\Lambda_c^+ \pi^-$ Decays in $p\bar{p}$ Collisions at
$\sqrt{s} = 1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {10},
Pages = {102002},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.102002},
Abstract = {http://arxiv.org/abs/0912.3566},
Doi = {10.1103/PhysRevLett.104.102002},
Key = {fds308482}
}
@article{fds308444,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of the ${B}^{-}$ lifetime using a simulation
free approach for trigger bias correction},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {3},
Pages = {032008},
Publisher = {American Physical Society},
Year = {2011},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.83.032008},
Abstract = {The collection of a large number of B-hadron decays to
hadronic final states at the CDF II Detector is possible due
to the presence of a trigger that selects events based on
track impact parameters. However, the nature of the
selection requirements of the trigger introduces a large
bias in the observed proper-decay-time distribution. A
lifetime measurement must correct for this bias, and the
conventional approach has been to use a Monte Carlo
simulation. The leading sources of systematic uncertainty in
the conventional approach are due to differences between the
data and the Monte Carlo simulation. In this paper, we
present an analytic method for bias correction without using
simulation, thereby removing any uncertainty due to the
differences between data and simulation. This method is
presented in the form of a measurement of the lifetime of
the B- using the mode B-→D0π -. The B- lifetime is
measured as τB -=1.663±0.023±0.015ps, where the first
uncertainty is statistical and the second systematic. This
new method results in a smaller systematic uncertainty in
comparison to methods that use simulation to correct for the
trigger bias. © 2011 American Physical Society.},
Doi = {10.1103/PhysRevD.83.032008},
Key = {fds308444}
}
@article{fds321184,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Measurement of the angular coefficients in Z-boson events
using electron and muon pairs from data taken at √s = 8
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)159},
Abstract = {The angular distributions of Drell-Yan charged lepton pairs
in the vicinity of the Z-boson mass peak probe the
underlying QCD dynamics of Z-boson production. This paper
presents a measurement of the complete set of angular
coefficients A0−7 describing these distributions in the
Z-boson Collins-Soper frame. The data analysed correspond to
20.3 fb−1 of pp collisions at s=8 TeV, collected by the
ATLAS detector at the CERN LHC. The measurements are
compared to the most precise fixed-order calculations
currently available (O(αs2)) and with theoretical
predictions embedded in Monte Carlo generators. The
measurements are precise enough to probe QCD corrections
beyond the formal accuracy of these calculations and to
provide discrimination between different parton-shower
models. A significant deviation from the (O(αs2))
predictions is observed for A0 − A2. Evidence is found for
non-zero A5,6,7, consistent with expectations.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP08(2016)159},
Key = {fds321184}
}
@article{fds308657,
Author = {Collaboration, CDF},
Title = {Measurement of the Associated ƒ× + ƒÝ„b Production
Cross Section in pp Collisions at = 1.8 TeV},
Journal = {Phys. Rev.},
Volume = {D60},
Number = {8},
Pages = {092003},
Year = {1999},
url = {http://dx.doi.org/10.1103/physrevlett.97.082004},
Abstract = {We present a measurement of the top quark pair production
cross section in pp collisions at square root of s = 1.96
TeV using 318 pb(-1) of data collected with the Collider
Detector at Fermilab. We select tt[over ] decays into the
final states enu+jets and mu nu+ jets, in which at least one
b quark from the t-quark decays is identified using a
secondary vertex-finding algorithm. Assuming a top quark
mass of 178 GeV/c2, we measure a cross section of 8.7 +/-
0.9(stat)(-0.9)+1.1(syst) pb. We also report the first
observation of tt[over ] with significance greater than
5sigma in the subsample in which both b quarks are
identified, corresponding to a cross section of
10.1(-1.4)+1.6(stat)(-1.3)+2.0(syst) pb.},
Doi = {10.1103/physrevlett.97.082004},
Key = {fds308657}
}
@article{fds331629,
Author = {Acosta, D and al, E},
Title = {Measurement of the average time-integrated mixing
probability of b-flavored hadrons produced at the
Tevatron},
Journal = {Phys. Rev.},
Volume = {D69},
Number = {1},
Pages = {012002},
Publisher = {American Physical Society (APS)},
Year = {2004},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.69.012002},
Abstract = {We have measured the number of like-sign (LS) and
opposite-sign (OS) lepton pairs arising from double
semileptonic decays of b and b-bar hadrons, pair produced at
the Fermilab Tevatron collider. The data samples were
collected with the Collider Detector at Fermilab during the
1992Ð1995 collider run by triggering on the existence of
µµ or eµ candidates in an event. The observed ratio of LS
to OS dileptons leads to a measurement of the average
time-integrated mixing probability of all produced
b-flavored hadrons which decay weakly, chi
-bar=0.152±0.007Ê(stat)±0.011Ê(syst), that is
significantly larger than the world average chi
-bar=0.118±0.005.},
Doi = {10.1103/PhysRevD.69.012002},
Key = {fds331629}
}
@article{fds308303,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau,
M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
RN},
Title = {Measurement of the azimuthal angle dependence of inclusive
jet yields in Pb+Pb collisions at √(sNN)=2.76 TeV with the
ATLAS detector.},
Journal = {Physical review letters},
Volume = {111},
Number = {15},
Pages = {152301},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.111.152301},
Abstract = {Measurements of the variation of inclusive jet suppression
as a function of relative azimuthal angle, Δφ, with
respect to the elliptic event plane provide insight into the
path-length dependence of jet quenching. ATLAS has measured
the Δφ dependence of jet yields in 0.14 nb(-1) of
√(s(NN))=2.76 TeV Pb+Pb collisions at the LHC for jet
transverse momenta p(T)>45 GeV in different collision
centrality bins using an underlying event subtraction
procedure that accounts for elliptic flow. The variation of
the jet yield with Δφ was characterized by the parameter,
v(2)(jet), and the ratio of out-of-plane (Δφ~π/2) to
in-plane (Δφ~0) yields. Nonzero v(2)(jet) values were
measured in all centrality bins for p(T)<160 GeV. The jet
yields are observed to vary by as much as 20% between
in-plane and out-of-plane directions.},
Doi = {10.1103/physrevlett.111.152301},
Key = {fds308303}
}
@article{fds308694,
Author = {Abulencia, and A, and others},
Title = {Measurement of the b jet cross section in events with a Z
boson in $p\bar{p}$ collisions at $\sqrt{s} =$
1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D74},
Number = {3},
Pages = {032008},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.74.032008},
Abstract = {A measurement of the inclusive bottom jet cross section is
presented for events containing a Z boson in p anti-p
collisions at s**(1/2) = 1.96 TeV using the Collider
Detector at Fermilab. Z bosons are identified in their
electron and muon decay modes, and b jets with E(t) > 20 GeV
and |eta| l+ l-) = 0.93 +/- 0.36 pb is found, where B(Z -->
l+ l-) is the branching ratio of the Z boson or gamma* into
a single flavor dilepton pair (e or mu) in the mass range
between 66 and 116 GeV/c2. The ratio of b jets to the total
number of jets of any flavor in the Z sample, within the
same kinematic range as the b jets, is 2.36 +/- 0.92\%.
Here, the uncertainties are the quadratic sum of statistical
and systematic uncertainties. Predictions made with NLO QCD
agree, within experimental and theoretical uncertainties,
with these measurements.},
Doi = {10.1103/PhysRevD.74.032008},
Key = {fds308694}
}
@article{fds308422,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
M and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann,
JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, H-C and Farrington, S and Feindt,
M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan,
N and Redondo, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T},
Title = {Measurement of the B(s)0 lifetime in fully and partially
reconstructed B(s)0→D(s)(-)(ϕπ(-))X decays in p¯p
collisions at √s=1.96 TeV.},
Journal = {Physical review letters},
Volume = {107},
Number = {27},
Pages = {272001},
Year = {2011},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.107.272001},
Abstract = {We present a measurement of the B(s)(0) lifetime in fully
and partially reconstructed B(s)(0)→D(s)(-)(ϕπ(-))X
decays in 1.3 fb(-1) collected in pp ¯ collisions at
√s=1.96 TeV by the CDF II detector at the Fermilab
Tevatron. We measure τ(B(s)(0))=1.518±0.041(stat)±0.027(syst) ps.
The ratio of this result and the world average B(0) lifetime
yields τ(B(s)(0))/τ(B(0))=0.99±0.03, which is in
agreement with recent theoretical predictions.},
Doi = {10.1103/physrevlett.107.272001},
Key = {fds308422}
}
@article{fds308912,
Author = {Abe, F and Albrow, M and Amidei, D and Anway-Wiese, C and Apollinari, G and Areti, H and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bolognesi, V and Bortoletto, D and Boswell,
C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman, J and Chiarelli, G and Chikamatsu, T and Cihangir, S and Clark, AG and Cobal,
M},
Title = {Measurement of the B+ and B0 meson lifetimes.},
Journal = {Physical review letters},
Volume = {72},
Number = {22},
Pages = {3456-3460},
Publisher = {American Physical Society (APS)},
Year = {1994},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.72.3456},
Abstract = {The lifetimes of the B+ and B0 mesons have been measured
using fully reconstructed decays. In a sample of ∼49
600J/ψ→μ+μ- decays recorded with the Collider Detector
at Fermilab, 148±16 B+ and 121±16B0 mesons have been
reconstructed using the silicon vertex detector. Unbinned
likelihood fits to the proper lifetime distributions of
these B mesons give τ+=1.61±0.16 (stat)±0.05 (syst) ps,
τ0=1.57±0.18 (stat) ±0.08 (syst) ps, and τ+/τ0=1.
02±0.16 (stat) ±0.05 (syst). © 1994 The American Physical
Society.},
Doi = {10.1103/physrevlett.72.3456},
Key = {fds308912}
}
@article{fds308650,
Author = {Abulencia, and A, and others},
Title = {Measurement of the B+ production cross section in p anti-p
collisions at s**(1/2) = 1960-GeV},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {5},
Pages = {012010},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.93.052001},
Abstract = {We present a new measurement of the B+ meson differential
cross section dsigma/dpT at sqrt(s)=1960 GeV. The data
correspond to an integrated luminosity of 739 pb-1 collected
with the upgraded CDF detector (CDF II) at the Fermilab
Tevatron collider. B+ candidates are reconstructed through
the decay B+-->J/psiK+, with J/psi-->µ+µ-. The integrated
cross section for producing B+ mesons with pT>=6 GeV/c and
|y|},
Doi = {10.1103/PhysRevD.93.052001},
Key = {fds308650}
}
@article{fds331637,
Author = {al, DAE},
Title = {Measurement of the B+ total cross section and B+
differential cross section do/dpT in pp collisions at
$\sqrt{s} = 1.8 TeV},
Journal = {Physical Review},
Volume = {D65},
Number = {5},
Pages = {052005},
Year = {2002},
url = {http://dx.doi.org/10.1103/PhysRevD.65.052005},
Abstract = {We present measurements of the [Formula Presented] meson
total cross section and differential cross section [Formula
Presented] The measurements use a [Formula Presented]
[Formula Presented] sample of [Formula Presented] collisions
at [Formula Presented] collected by the CDF detector.
Charged B meson candidates are reconstructed through the
decay [Formula Presented] with [Formula Presented] The total
cross section, measured in the central rapidity region
[Formula Presented] for [Formula Presented] is [Formula
Presented] The measured differential cross section is
substantially larger than typical QCD predictions calculated
to next-to-leading order. © 2002 The American Physical
Society.},
Doi = {10.1103/PhysRevD.65.052005},
Key = {fds331637}
}
@article{fds308877,
Author = {al, FAE},
Title = {Measurement of the B- and (B)over-bar(0) meson lifetimes
using semileptonic decays},
Journal = {Phys. Rev. Lett.},
Volume = {76},
Number = {24},
Pages = {4462-4467},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevLett.76.4462},
Abstract = {The lifetimes of the B- and B−0 mesons are measured using
the partially reconstructed semileptonic decays
B−→D1-v−X, where D is either a D0 or D*+ meson. The
data were collected by the CDF detector at the Fermilab
Tevatron collider during 1992-1993 and correspond to 19.3
pb−1 of p−p collisions at s = 1.8 TeV. We measure the
decay length distributions and find the lifetimes to be
τ(B−) = 1.56±0.13±0.06 ps and τ(B−0) =
1.54±0.08±0.06 ps, and the ratio of lifetimes to be
τ(B−)/τ(B−0) = 1.01±0.11±0.02, where the first
uncertainties are statistical and the second are systematic.
© 1996 The American Physical Society.},
Doi = {10.1103/PhysRevLett.76.4462},
Key = {fds308877}
}
@article{fds308559,
Author = {Aaltonen, T and others},
Title = {Measurement of the b-hadron production cross section using
decays to mu[sup -]D[sup 0]X final states in p[overline p]
collisions at sqrt(s) = 1.96 TeV},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {9},
Pages = {092003},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.092003},
Abstract = {We report a measurement of the production cross section for
b hadrons in pp̄ collisions at s=1.96TeV. Using a data
sample derived from an integrated luminosity of 83pb-1
collected with the upgraded Collider Detector (CDF II) at
the Fermilab Tevatron, we analyze b hadrons, Hb, partially
reconstructed in the semileptonic decay mode Hb→μ-D0X.
Our measurement of the inclusive production cross section
for b hadrons with transverse momentum pT>9GeV/c and
rapidity |y|<0.6 is σ=1.30μb±0.05μb(stat)±0.
14μb(syst)±0.07μb(B), where the uncertainties are
statistical, systematic, and from branching fractions,
respectively. The differential cross sections dσ/dpT are
found to be in good agreement with recent measurements of
the Hb cross section and well described by fixed-order
next-to-leading logarithm predictions. © 2009 The American
Physical Society.},
Doi = {10.1103/PhysRevD.79.092003},
Key = {fds308559}
}
@article{fds308895,
Author = {al, FAE},
Title = {Measurement of the b-meson differential cross-section
d-sigma/dp(t) in p(p)over-bar collisions at root-s=1.8
tev},
Journal = {Phys. Rev. Lett.},
Volume = {75},
Number = {8},
Pages = {1451-1455},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevLett.75.1451},
Abstract = {This paper presents the first direct measurement of the B
meson differential cross section dσ/dpT in pp̄ collisions
at s=1.8 TeV using a sample of 19.3±0.7 pb-1 accumulated by
the Collider Detector at Fermilab. The cross section is
measured in the central rapidity region |y|<1 for pTB>6.0
GeV /c by fully reconstructing the B meson decays
B+→J/ψK+ and B0→J/ψK*0892, where J/ψ→μ+μ- and
K*0→K+π-. A comparison is made to the theoretical QCD
prediction calculated at next-to-leading order. © 1995 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.75.1451},
Key = {fds308895}
}
@article{fds308892,
Author = {al, FAE},
Title = {Measurement of the b-s meson lifetime},
Journal = {Phys. Rev. Lett.},
Volume = {74},
Number = {25},
Pages = {4988-4992},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevLett.74.4988},
Abstract = {The lifetime of the Bs meson is measured using the
semileptonic decay Bs→Ds-+νX. The data sample consists of
19.3 pb-1 of pp̄ collisions at s=1.8 TeV collected by the
Collider Detector at Fermilab during 1992-1993. There are
76±8 +Ds- signal events where the Ds is identified via the
decay Ds-→φπ-, φ→K+K-. Using these events, the Bs
meson lifetime is determined to be τs=1.42-0.23+0.27(stat)±0.11(syst)
ps. A measurement of the Bs lifetime in a low statistics
sample of exclusive Bs→J/ψ φ decays is also presented in
this paper. © 1995 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.74.4988},
Key = {fds308892}
}
@article{fds308659,
Author = {Abulencia, and A, and others},
Title = {Measurement of the B/s0 anti-B/s0 oscillation
frequency},
Journal = {Phys. Rev. Lett.},
Volume = {97},
Number = {6},
Pages = {062003},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.97.062003},
Abstract = {We measure the masses of $b$ hadrons in exclusively
reconstructed final states containing a $J/\psi\to\mu^-\mu^+$
decay using $\rm 220 pb^{-1}$ of data collected by the CDF
II experiment. We find: m(B^+) = 5279.10 \pm 0.41_{(stat.)}
\pm 0.36_{(sys.)} MeVcc, m(B^0) = 5279.63 \pm 0.53_{(stat.)}
\pm 0.33_{(sys.)} MeVcc, m(B^0_s) = 5366.01 \pm
0.73_{(stat.)} \pm 0.33_{(sys.)} MeVcc, m(\Lambda^0_b) =
5619.7 \pm 1.2_{(stat.)} \pm 1.2_{(sys.)} MeVcc. m(B^+) -
m(B^0) = -0.53 \pm 0.67_{(stat.)} \pm 0.14_{(sys.)} MeVcc,
m(B^0_s) - m(B^0) = 86.38 \pm 0.90_{(stat.)} \pm
0.06_{(sys.)} MeVcc m(\Lambda^0_b) - m(B^0) = 339.2 \pm
1.4_{(stat.)} \pm 0.1_{(sys.)} MeVcc. The measurements of
the $B^0_s$, $\Lambda^0_b$ mass, $m(B^0_s)-m(B^0)$ and
$m(\Lambda^0_b)-m(B^0)$ mass difference are of better
precision than the current world averages.},
Doi = {10.1103/physrevlett.97.062003},
Key = {fds308659}
}
@article{fds308813,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh,
SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips,
TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni,
A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt,
MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill,
A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok,
K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima,
R and Takikawa, K and Tanaka, M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko,
M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar,
R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh,
GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of the Bd0-B̄d0
flavor oscillation frequency and study of same side flavor
tagging of B mesons in pp̄ collisions},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {59},
Number = {3},
Pages = {1-41},
Year = {1999},
ISSN = {0556-2821},
Abstract = {Bd0-B̄d0 oscillations are observed in "self-tagged" samples
of partially reconstructed B mesons decaying into a lepton
and a charmed meson collected in pp̄ collisions at √s=1.8
TeV. A flavor tagging technique is employed which relies
upon the correlation between the flavor of B mesons and the
charge of a nearby particle. We measure the flavor
oscillation frequency to be Δmd=0.471-0.068+0.078±0.034
ps-1. The tagging method is also demonstrated in exclusive
samples of Bu+→J/ψK+ and Bd0→J/ψK*0(892), where
similar flavor-charge correlations are observed. The tagging
characteristics of the various samples are compared with
each other, and with Monte Carlo simulations.},
Key = {fds308813}
}
@article{fds308814,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari,
C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Breccia, L and Bromberg,
C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell,
M and Caner, A and Carithers, W and Carlsmith, D and Cassada, J and Castro,
A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Cropp, R and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Dolce, G and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti,
C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman,
J and Friedman, J and Frisch, H and Fukui, Y and Gadomski, S and Galeotti,
S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel,
AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz,
E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato,
Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart,
R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster,
M and Lanzoni, M and Latino, G and LeCompte, T and IV, AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer,
N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Partos,
D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara,
L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi,
F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw,
NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith,
C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella,
F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka, M and Tannenbaum,
B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto,
Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk,
W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal,
R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner,
RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei,
C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli,
S},
Title = {Measurement of the Bd0B̄d0
oscillation frequency using dimuon data in pp̄ collisions
at √s = 1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {60},
Number = {5},
Pages = {1-6},
Year = {1999},
Abstract = {We present a measurement of the mass difference Δmd of the
two Bd0 mass eigenstates. We use a flavor tagging method
based on the lepton charge, in a sample of events with two
muons at low transverse momentum. The sample corresponds to
an integrated luminosity of 90 pb-1 collected by the
Collider Detector at Fermilab. The result obtained is
Δmd=0.503±0.064(stat)±0.071(syst) ps-1. ©1999 The
American Physical Society.},
Key = {fds308814}
}
@article{fds308812,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh,
SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips,
TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni,
A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt,
MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill,
A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok,
K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima,
R and Takikawa, K and Tanaka, M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko,
M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar,
R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh,
GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of the BS0 meson lifetime
using semileptonic decays},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {59},
Number = {3},
Pages = {1-14},
Year = {1999},
Abstract = {The lifetime of the BS0 meson is measured using the
semileptonic decay BS0→DS-l+νX. The data sample consists
of about 110 pb-1 of pp̄ collisions at √s=1.8 TeV
collected by the CDF detector at Fermilab. Four different
DS- decay modes are reconstructed resulting in approximately
600 DS-l+ signal events. The BS0 meson lifetime is
determined to be τ(BS0)=(1.36±0.09-0.05+0.06) ps, where
the first and second uncertainties are statistical and
systematic, respectively. The BS0 meson decay length
distribution is examined for a lifetime difference ΔΓ/Γ
between the two mass eigenstates of the BS0 meson. An upper
limit of ΔΓ/Γ<0.83 is set at the 95% confidence
level.},
Key = {fds308812}
}
@article{fds308829,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
R and Engels, E and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handa,
T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris,
RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster,
M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer,
N and Long, O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh,
SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips,
TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni,
A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt,
MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill,
A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok,
K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima,
R and Takikawa, K and Tanaka, M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko,
M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar,
R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh,
GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of the B- and B̄0meson
lifetimes using semileptonic decays},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {58},
Number = {9},
Pages = {920021-9200212},
Year = {1998},
ISSN = {0556-2821},
Abstract = {The lifetimes of the B- and B̄0 mesons are measured using
the partially reconstructed semileptonic decays B̄ → Dl-
v̄X, where D0 is either a D0 or D*+ meson. The data were
collected by the CDF detector at the Fermilab Tevatron
collider during 1992-1995 and correspond to about 110 pb-1
of pp collisions at √s = 1.8 TeV. We measure decay lengths
and extract the lifetimes to be τ(B-) =
1.637±0.058-0.043+0.045 ps and τ(B̄0) =
1.474±0.039-0.051+0.052 ps, and the ratio of the lifetimes
to be τ(B-)/τ(B̄0) = 1.110±0.056-0.030+0.033, where the
first uncertainties are statistical and the second are
systematic.},
Key = {fds308829}
}
@article{fds308842,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal,
M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli,
M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
R and Jr, EE and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Galeotti, S and Gallinaro,
M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn,
SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara,
K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi,
E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber,
TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Kondo, K and Köngeter, A and Konigsberg, J and Kordas, K and Korytov, A and Kovacs,
E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi,
E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pondrom,
L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spiegel, L and Spinella, F and Spiropulu, M and Stanco,
L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
N and Uchida, T and Ukegawa, F and Brink, SCVD and Vejcik, S and Velev, G and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang,
MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkinson,
R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of the B0-B̄0 oscillation
frequency using π-B meson charge-flavor correlations in
pp̄ collisions at √s= 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {80},
Number = {10},
Pages = {2057-2062},
Year = {1998},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.2057},
Abstract = {We present a measurement of the B0 ↔ B̄0 oscillalion
frequency using a flavor tagging method based on
correlations of B meson flavor with the charge of other
particles produced in pp̄ collisions at √s = 1.8 TeV.
Such correlations are expected to arise from b quark
hudronization and from B** decays. We partially reconstruct
B mesons using the semileptonic decays B0 → D(*)-X and B+
rarr; -D̄0X. From the oscillation frequency, we obtain the
mass difference between the two B0 mass eigenstates. Δmd =
0.471 -0.068+0.078(stat) ± 0.034(syst)ℏ ps-1, and measure
the efficiency and purity of this flavor tagging method for
both charged and neutral B mesons.},
Doi = {10.1103/PhysRevLett.80.2057},
Key = {fds308842}
}
@article{fds308820,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Antos, J and Apollinari, G and Arisawa,
T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge,
JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker,
C and Bloom, K and Blusk, S and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl,
A and Brink, SVD and Bromberg, C and Brunner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlson,
J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng,
MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze,
G and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Cobal, M and Cocca, E and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Costa, JGD and Costanzo, D and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold, M and Goldstein,
J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser,
J and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck,
C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara,
H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov,
A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and IV,
AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Meschi, E and Mesropian, C and Miao, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Moggi, N and Moore, E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman, J and Nahn,
S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti,
R and Papadimitriou, V and Pappas, SP and Parri, A and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos,
A and Pondrom, L and Pope, G and Prokoshin, F and Proudfoot, J and Ptohos,
F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takashima, R and Takikawa, K and Tanaka, M and Takano, T and Tannenbaum,
B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Ukegawa, F and Valls, J and III, SV and Velev, G and Vidai, R and Vilar, R and Vologouev,
I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Watts,
T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu,
I and Yu, S and Zanetti, A and Zetti, F and Zucchelli,
S},
Title = {Measurement of the B0B̄0 oscillation
frequency using l-D*+ pairs and lepton
flavor tags},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {60},
Number = {11},
Pages = {1-12},
Year = {1999},
Abstract = {The oscillation frequency Δmd of B0B̄0 mixing is measured
using the partially reconstructed semileptonic decay
B̄0→l-ν̄D*+X. The data sample was collected with the
CDF detector at the Fermilab Tevatron collider during
1992-1995 by triggering on the existence of two lepton
candidates in an event, and corresponds to about 110 pb-1 of
p̄p collisions at √s=1.8 TeV. We estimate the proper
decay time of the B̄0meson from the measured decay length
and reconstructed momentum of the l-D*+ system. The charge
of the lepton in the final state identifies the flavor of
the B̄0 meson at its decay. The second lepton in the event
is used to infer the flavor of the B̄0 meson at production.
We measure the oscillation frequency to be Δmd=0.516
±0.099-0.035+0.029 ps-1, where the first uncertainty is
statistical and the second is systematic. ©1999 The
American Physical Society.},
Key = {fds308820}
}
@article{fds362146,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and DiTuro, P and Dorr, C and Donati, S and Donega, M and Dong, P and Donini,
J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris, N and Giolo, K and Giordani, M and Giromini,
P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos,
G and Goncharov, M and Gonzalez, O and Gorelov, I and Goshaw, AT and Gotra,
Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Hahn, K and Halkiadakis,
E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer, A and Heinemann,
B and Heinrich, J and Herndon, M and Hidas, D and Hill, CS and Hirschbuehl,
D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi,
G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon,
T and Kang, J and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto,
A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mulmenstadt, J and Mukherjee, A and Muller, T and Mumford, R and Murat,
P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg,
K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou,
V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel,
NV and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli,
S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P},
Title = {Measurement of the Bc+ meson lifetime using the decay mode
Bc+→J/ψe+νe},
Journal = {Physical Review Letters},
Volume = {97},
Number = {1},
Pages = {012002},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevLett.97.012002},
Abstract = {We present a measurement of the Bc+ meson lifetime in the
decay mode Bc+→J/ψe+νe using the Collider Detector at
Fermilab II detector at the Fermilab Tevatron Collider. From
a sample of about 360pb-1 of pp̄ collisions at s=1.96TeV,
we reconstruct J/ψe+ pairs with invariant mass in the
kinematically allowed range 4<MJ/ψe<6GeV/c2. A fit to
the decay-length distribution of 238 signal events yields a
measured Bc+ meson lifetime of 0.463+0.073-0.065(stat)±0.036(syst)ps.
© 2006 The American Physical Society.},
Doi = {10.1103/PhysRevLett.97.012002},
Key = {fds362146}
}
@article{fds308356,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and D'Errico, M},
Title = {Measurement of the Bc-meson lifetime in the decay
Bc-→J/ψπ},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.87.011101},
Abstract = {The lifetime of the Bc- meson is measured using 272
exclusive Bc-→J/ψ(→μ+μ-)π- decays reconstructed in
data from proton-antiproton collisions corresponding to an
integrated luminosity of 6.7 fb-1 recorded by the CDF II
detector at the Fermilab Tevatron. The lifetime of the Bc-
meson is measured to be τ(Bc-)=0.452±0.048(stat)±0.027(syst)
ps. This is the first measurement of the Bc- meson lifetime
in a fully reconstructed hadronic channel, and it agrees
with previous results and has comparable precision. © 2013
American Physical Society.},
Doi = {10.1103/PhysRevD.87.011101},
Key = {fds308356}
}
@article{fds308377,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grillo, L and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of the bottom-strange meson mixing phase in the
full CDF data set.},
Journal = {Physical review letters},
Volume = {109},
Number = {17},
Pages = {171802},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.109.171802},
Abstract = {We report a measurement of the bottom-strange meson mixing
phase β(s) using the time evolution of B(s)(0)→J/ψ(→μ(+)μ(-))φ(→K(+)K(-))
decays in which the quark-flavor content of the
bottom-strange meson is identified at production. This
measurement uses the full data set of proton-antiproton
collisions at √s=1.96 TeV collected by the Collider
Detector experiment at the Fermilab Tevatron, corresponding
to 9.6 fb(-1) of integrated luminosity. We report confidence
regions in the two-dimensional space of β(s) and the
B(s)(0) decay-width difference ΔΓ(s) and measure
β(s)∈[-π/2,-1.51]∪[-0.06,0.30]∪[1.26,π/2] at the
68% confidence level, in agreement with the standard model
expectation. Assuming the standard model value of β(s), we
also determine ΔΓ(s)=0.068±0.026(stat)±0.009(syst)
ps(-1) and the mean B(s)(0) lifetime τ(s)=1.528±0.019(stat)±0.009(syst)
ps, which are consistent and competitive with determinations
by other experiments.},
Doi = {10.1103/physrevlett.109.171802},
Key = {fds308377}
}
@article{fds308875,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Bondreau, J and Breccia, L and Bromberg,
C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane,
D and Cronin-Hennessy, D and Culbertson, R and Daniels, T and DeJongh,
F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Dunn, A and Eddy,
N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Errede, D and Errede, S and Fan, Q and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman,
J and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti,
S and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gladney, L and Glenzinski, D and Gold, M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Hardman, AD and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Hayashi, E and Heinrich, J and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway, L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes, R and Huston, J and Huth, J and Hylen, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and Jensen, H and Joshi, U and Kadel, RW and Kajfasz,
E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato,
Y and Keaffaber, TA and Keeble, L and Kelley, K and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian,
H and Keyvan, F and Kharadia, B and Kim, BJ and Kim, DH and Kim, HS and Kim,
SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Korytov, A and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuwabara, T and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca,
N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis,
JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lu, J and Lucchesi, D and Lukens, P and Lusin,
S and Lys, J and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin,
A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Mitsushio, H and Miyamoto, T and Miyashita, S and Moggi, N and Morita,
Y and Mueller, J and Mukherjee, A and Muller, T and Murat, P and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ninomiya, M and Nodulman, L and Oh, SH and Ohl, KE and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Oliveira, R and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Park, S and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett,
R and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Romano, J and Rosenson, L and Roser, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scribano, A and Segler,
S and Seidel, S and Seiya, Y and Sganos, G and Shapiro, MD and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Snider,
FD and Song, T and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
A and Strahl, K and Strait, J and Ströhmer, R and Stuart, D and Sullivan,
G and Soumarokov, A and Sumorok, K and Suzuki, J and Takada, T and Takahashi, T and Takano, T and Takikawa, K and Tamura, N and Tartarelli,
F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov, A and Tkaczyk,
S and Toback, D and Tollefson, K and Tollestrup, A and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Uemura, N and Ukegawa, F and Unal, G and Vails, J and Brink, SCVD and Vejcik, S and Velev, G and Vidal, R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, N and Wang, C and Wang, CH and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef, C and Yoshida, T and Yovanovitch, D and Yu, I and Yu, L and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, W and Zucchelli,
S},
Title = {Measurement of the branching fraction B(Bu+→J/ψπ+)
and search for Bc+→J/ψπ+},
Journal = {Physical Review Letters},
Volume = {77},
Number = {26},
Pages = {5176-5181},
Year = {1996},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.77.5176},
Abstract = {We report on a measurement of the branching fraction of the
Cabibbo-suppressed decay Bu+→J/ψπ+ , where
J/ψ→μ+μ-. The data were collected by the Collider
Detector at Fermilab during 1992-1995 and correspond to an
integrated luminosity of 110 pb-1 in p̄p collisions at √s
= 1.8 TeV. A signal of 289+10 events is observed and we
determine the ratio of branching fractions
B(Bu+→J/ψπ+)/B(Bu+→J/ψK+) to be [5.0-1.7+1.9(stat) ±
0.1(syst)]%. Using the world average value for
B(Bu+→J/ψK+), we calculate the branching fraction
B(Bu+→J/ψπ+) to be (5.0-1.9+2.1) × 10-5. We also search
for the decay Bc+→J/ψπ+ and report a 95% confidence
level limit on σ(Bc+)B(Bc+→ J/ψπ+)/σ(Bu+)B(Bu+→J/ψK+)
as a function of the Bc+ lifetime.},
Doi = {10.1103/PhysRevLett.77.5176},
Key = {fds308875}
}
@article{fds308414,
Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli,
M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F and D'errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan,
G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giakoumopoulou,
V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh,
SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Poukhov,
O and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro,
A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Squillacioti, P and Stancari, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, WM and Yeh, GP and Yi, K and Yoh,
J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zucchelli, S},
Title = {Measurement of the branching fraction B(Λb0→Λc+π
-π +π -) at
CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.85.032003},
Abstract = {We report an analysis of the Λb0→Λc+π -π +π - decay
in a data sample collected by the CDF II detector at the
Fermilab Tevatron corresponding to 2.4fb -1 of integrated
luminosity. We reconstruct the currently largest samples of
the decay modes Λb0→Λ c(2595) +π - (with Λ c(2595)
+→Λc+π +π -), Λb0→Λ c(2625) +π - (with Λ c(2625)
+→Λc+π +π -), Λb0→Σ c(2455) ++π -π - (with Σ
c(2455) ++→Λc+π +), and Λb0→Σ c(2455)0π +π - (with
Σ c(2455)0→Λc+π -) and measure the branching fractions
relative to the Λb0→Λc+π - branching fraction. We
measure the ratio B(Λb0→Λc+π -π +π -)/B(Λb0→Λc+π
-)=3.04±0.33(stat)-0.55+0.70(syst) which is used to derive
B(Λb0→Λc+π -π +π -)= (26.8-11.2+11.9)×10 -3. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.85.032003},
Key = {fds308414}
}
@article{fds314188,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of the branching ratio Γ(Λb0→ψ(2S)Λ0)/Γ(Λb0→J/ψΛ0)
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {751},
Pages = {63-80},
Publisher = {Elsevier BV},
Year = {2015},
Month = {December},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2015.10.009},
Abstract = {An observation of the Λb0→ψ(2S)Λ0 decay and a
comparison of its branching fraction with that of the
Λb0→J/ψΛ0 decay has been made with the ATLAS detector
in proton–proton collisions at s=8 TeV at the LHC using an
integrated luminosity of 20.6 fb−1. The J/ψ and ψ(2S)
mesons are reconstructed in their decays to a muon pair,
while the Λ0→pπ− decay is exploited for the Λ0 baryon
reconstruction. The Λb0 baryons are reconstructed with
transverse momentum pT>10 GeV and pseudorapidity |η|<2.1.
The measured branching ratio of the Λb0→ψ(2S)Λ0 and
Λb0→J/ψΛ0 decays is Γ(Λb0→ψ(2S)Λ0)/Γ(Λb0→J/ψΛ0)=0.501±0.033(stat)±0.019(syst),
lower than the expectation from the covariant quark
model.},
Doi = {10.1016/j.physletb.2015.10.009},
Key = {fds314188}
}
@article{fds321359,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
M},
Title = {Measurement of the centrality and pseudorapidity dependence
of the integrated elliptic flow in lead-lead collisions at
[Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {8},
Pages = {2982},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-2982-4},
Abstract = {The integrated elliptic flow of charged particles produced
in Pb+Pb collisions at [Formula: see text] TeV has been
measured with the ATLAS detector using data collected at the
Large Hadron Collider. The anisotropy parameter, [Formula:
see text], was measured in the pseudorapidity range
[Formula: see text] with the event-plane method. In order to
include tracks with very low transverse momentum [Formula:
see text], thus reducing the uncertainty in [Formula: see
text] integrated over [Formula: see text], a [Formula: see
text] data sample recorded without a magnetic field in the
tracking detectors is used. The centrality dependence of the
integrated [Formula: see text] is compared to other
measurements obtained with higher [Formula: see text]
thresholds. The integrated elliptic flow is weakly
decreasing with [Formula: see text]. The integrated
[Formula: see text] transformed to the rest frame of one of
the colliding nuclei is compared to the lower-energy RHIC
data.},
Doi = {10.1140/epjc/s10052-014-2982-4},
Key = {fds321359}
}
@article{fds315436,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, J-F and Argyropoulos,
S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
P and Balli, F and Banas, E and Banerjee, S and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho
Toro, R and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa,
A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavez
Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Coggeshall, J and Cole, B and Cole, S and Colijn, AP and Collins-Tooth, C and Collot, J and Colombo,
T},
Title = {Measurement of the centrality dependence of the
charged-particle pseudorapidity distribution in proton-lead
collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {4},
Pages = {199},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4002-3},
Abstract = {The centrality dependence of the mean charged-particle
multiplicity as a function of pseudorapidity is measured in
approximately 1 [Formula: see text]b[Formula: see text] of
proton-lead collisions at a nucleon-nucleon centre-of-mass
energy of [Formula: see text] [Formula: see text] using the
ATLAS detector at the Large Hadron Collider. Charged
particles with absolute pseudorapidity less than 2.7 are
reconstructed using the ATLAS pixel detector. The [Formula:
see text] collision centrality is characterised by the total
transverse energy measured in the Pb-going direction of the
forward calorimeter. The charged-particle pseudorapidity
distributions are found to vary strongly with centrality,
with an increasing asymmetry between the proton-going and
Pb-going directions as the collisions become more central.
Three different estimations of the number of nucleons
participating in the [Formula: see text] collision have been
carried out using the Glauber model as well as two
Glauber-Gribov inspired extensions to the Glauber model.
Charged-particle multiplicities per participant pair are
found to vary differently for these three models,
highlighting the importance of including colour fluctuations
in nucleon-nucleon collisions in the modelling of the
initial state of [Formula: see text] collisions.},
Doi = {10.1140/epjc/s10052-016-4002-3},
Key = {fds315436}
}
@article{fds376312,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Aktas, S and Al Khoury and K and Alberghi,
GL and Albert, J and Albicocco, P and Albouy, GL and Alderweireldt, S and Alegria, ZL and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arbiol Val and SJ and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling,
J-H and Arnaez, O and Arnold, H and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Baer, TM and Bagnaia, P and Bahmani, M and Bahner, D and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barel, MZ and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beaucamp, JY and Beauchemin, PH and Becherer, F and Bechtle, P and Beck,
HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berrocal Guardia and A and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhalla, NK and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
PA and Brüers, B and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlotto, JI and Carlson,
BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos,
F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chakraborty, D and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi,
K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Clark, A},
Title = {Measurement of the Centrality Dependence of the Dijet Yield
in p+Pb Collisions at sqrt[s_{NN}]=8.16 TeV with the
ATLAS Detector.},
Journal = {Physical review letters},
Volume = {132},
Number = {10},
Pages = {102301},
Year = {2024},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.132.102301},
Abstract = {ATLAS measured the centrality dependence of the dijet yield
using 165 nb^{-1} of p+Pb data collected at
sqrt[s_{NN}]=8.16 TeV in 2016. The event centrality,
which reflects the p+Pb impact parameter, is characterized
by the total transverse energy registered in the Pb-going
side of the forward calorimeter. The central-to-peripheral
ratio of the scaled dijet yields, R_{CP}, is evaluated, and
the results are presented as a function of variables that
reflect the kinematics of the initial hard parton scattering
process. The R_{CP} shows a scaling with the Bjorken x of
the parton originating from the proton, x_{p}, while no such
trend is observed as a function of x_{Pb}. This analysis
provides unique input to understanding the role of small
proton spatial configurations in p+Pb collisions by covering
parton momentum fractions from the valence region down to
x_{p}∼10^{-3} and x_{Pb}∼4×10^{-4}.},
Doi = {10.1103/physrevlett.132.102301},
Key = {fds376312}
}
@article{fds321254,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Measurement of the charge asymmetry in dileptonic decays of
top quark pairs in pp collisions at √s = 7 TeV using the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {5},
Publisher = {Springer Nature},
Year = {2015},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2015)061},
Abstract = {A measurement of the top-antitop (tt¯) charge asymmetry is
presented using data corresponding to an integrated
luminosity of 4.6 fb−1 of LHC pp collisions at a
centreof-mass energy of 7 TeV collected by the ATLAS
detector. Events with two charged leptons, at least two jets
and large missing transverse momentum are selected. Two
observables are studied: ACℓℓ based on the identified
charged leptons, and (Formula Presented.), based on the
reconstructed tt final state. The asymmetries are measured
to be (Formula Presented.). The measured values are in
agreement with the Standard Model predictions.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP05(2015)061},
Key = {fds321254}
}
@article{fds375914,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V},
Title = {Measurement of the charge asymmetry in top-quark pair
production in association with a photon with the ATLAS
experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137848},
Abstract = {A measurement of the charge asymmetry in top-quark pair
(tt¯) production in association with a photon is presented.
The measurement is performed in the single-lepton tt¯ decay
channel using proton–proton collision data collected with
the ATLAS detector at the Large Hadron Collider at CERN at a
centre-of-mass-energy of 13 TeV during the years
2015–2018, corresponding to an integrated luminosity of
139 fb−1. The charge asymmetry is obtained from the
distribution of the difference of the absolute rapidities of
the top quark and antiquark using a profile likelihood
unfolding approach. It is measured to be AC=−0.003±0.029
in agreement with the Standard Model expectation.},
Doi = {10.1016/j.physletb.2023.137848},
Key = {fds375914}
}
@article{fds323675,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard,
CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman,
JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
Title = {Measurement of the charge asymmetry in top-quark pair
production in the lepton-plus-jets final state in pp
collision data at [Formula: see text] with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {87},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-3910-6},
Abstract = {This paper reports inclusive and differential measurements
of the [Formula: see text] charge asymmetry [Formula: see
text] in [Formula: see text] of [Formula: see text][Formula:
see text] collisions recorded by the ATLAS experiment at the
Large Hadron Collider at CERN. Three differential
measurements are performed as a function of the invariant
mass, transverse momentum and longitudinal boost of the
[Formula: see text] system. The [Formula: see text] pairs
are selected in the single-lepton channels (<i>e</i> or
[Formula: see text]) with at least four jets, and a
likelihood fit is used to reconstruct the [Formula: see
text] event kinematics. A Bayesian unfolding procedure is
performed to infer the asymmetry at parton level from the
observed data distribution. The inclusive [Formula: see
text] charge asymmetry is measured to be [Formula: see text]
(stat. [Formula: see text] syst.). The inclusive and
differential measurements are compatible with the values
predicted by the Standard Model.},
Doi = {10.1140/epjc/s10052-016-3910-6},
Key = {fds323675}
}
@article{fds321225,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Akesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of the correlation between flow harmonics of
different order in lead-lead collisions at √sNN
= 2.76 TeV with the ATLAS detector},
Journal = {Physical Review C - Nuclear Physics},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevC.92.034903},
Abstract = {Correlations between the elliptic or triangular flow
coefficients vm (m = 2 or 3) and other flow harmonics vn (n
= 2 to 5) are measured using √sNN = 2.76 TeV Pb + Pb
collision data collected in 2010 by the ATLAS experiment at
the LHC, corresponding to an integrated luminosity of 7
μb−1. The vm-vn correlations are measured in midrapidity
as a function of centrality, and, for events within the same
centrality interval, as a function of event ellipticity or
triangularity defined in a forward rapidity region. For
events within the same centrality interval, v3 is found to
be anticorrelated with v2 and this anticorrelation is
consistent with similar anticorrelations between the
corresponding eccentricities, ∊2 and ∊3. However, it is
observed that v4 increases strongly with v2, and v5
increases strongly with both v2 and v3. The trend and
strength of the vm-vn correlations for n = 4 and 5 are found
to disagree with ∊m-∊n correlations predicted by
initial-geometry models. Instead, these correlations are
found to be consistent with the combined effects of a linear
contribution to vn and a nonlinear term that is a function
of v22 or of v2v3, as predicted by hydrodynamic models. A
simple two-component fit is used to separate these two
contributions. The extracted linear and nonlinear
contributions to v4 and v5 are found to be consistent with
previously measured event-plane correlations.},
Doi = {10.1103/PhysRevC.92.034903},
Key = {fds321225}
}
@article{fds375940,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames,
CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche,
CS and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Measurement of the CP properties of Higgs boson interactions
with τ -leptons with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11583-y},
Abstract = {A study of the charge conjugation and parity (CP) properties
of the interaction between the Higgs boson and τ -leptons
is presented. The study is based on a measurement of CP
-sensitive angular observables defined by the visible decay
products of τ -leptons produced in Higgs boson decays. The
analysis uses 139 fb- 1of proton–proton collision data
recorded at a centre-of-mass energy of s=13 TeV with the
ATLAS detector at the Large Hadron Collider. Contributions
from CP -violating interactions between the Higgs boson and
τ -leptons are described by a single mixing angle parameter
ϕτin the generalised Yukawa interaction. Without
constraining the H→ ττ signal strength to its expected
value under the Standard Model hypothesis, the mixing angle
ϕτis measured to be 9∘± 16∘, with an expected value
of 0∘± 28∘at the 68% confidence level. The pure CP -odd
hypothesis is disfavoured at a level of 3.4 standard
deviations. The results are compatible with the predictions
for the Higgs boson in the Standard Model.},
Doi = {10.1140/epjc/s10052-023-11583-y},
Key = {fds375940}
}
@article{fds308404,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Bousson, N and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
Title = {Measurement of the CP-violating phase βsJ/ψ in Bs0→J/ψ
decays with the CDF II detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.85.072002},
Abstract = {We present a measurement of the CP-violating parameter
βsJ/ψ using approximately 6500 Bs0→J/ψ decays
reconstructed with the CDF II detector in a sample of pp̄
collisions at √s=1.96TeV corresponding to 5.2fb -1
integrated luminosity produced by the Tevatron collider at
Fermilab. We find the CP-violating phase to be within the
range βsJ/ψ [0.02,0.52] [1.08,1.55] at 68% confidence
level where the coverage property of the quoted interval is
guaranteed using a frequentist statistical analysis. This
result is in agreement with the standard model expectation
at the level of about one Gaussian standard deviation. We
consider the inclusion of a potential S-wave contribution to
the Bs0→J/ψK +K - final state which is found to be
negligible over the mass interval 1.009<m(K +K
-)<1.028GeV/c2. Assuming the standard model prediction for
the CP-violating phase βsJ/ψ, we find the Bs0 decay width
difference to be ΔΓ s=0.075±0.035(stat) ±0.006(syst)ps
-1. We also present the most precise measurements of the Bs0
mean lifetime τ(Bs0)=1.529±0.025(stat) ±0.012(syst)ps,
the polarization fractions |A 0(0)|2=0. 524±0.013(stat)±0.015(syst)
and |A -(0)|2=0. 231±0.014(stat)±0.015(syst), as well as
the strong phase δ -=2.95±0.64(stat)±0.07(syst)rad. In
addition, we report an alternative Bayesian analysis that
gives results consistent with the frequentist approach. ©
2012 American Physical Society.},
Doi = {10.1103/PhysRevD.85.072002},
Key = {fds308404}
}
@article{fds365407,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
Title = {Measurement of the CP-violating phase ϕs in
Bs0→J/ψϕ decays in ATLAS at 13 TeV},
Journal = {European Physical Journal C},
Volume = {81},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09011-0},
Abstract = {A measurement of the Bs0→J/ψϕ decay parameters using
80.5fb-1 of integrated luminosity collected with the ATLAS
detector from 13 Te proton–proton collisions at the LHC
is presented. The measured parameters include the
CP-violating phase ϕs, the width difference Δ Γ s between
the Bs0 meson mass eigenstates and the average decay width
Γ s. The values measured for the physical parameters are
combined with those from 19.2fb-1 of 7 and 8 Te data,
leading to the following: ϕs=-0.087±0.036(stat.)±0.021(syst.)radΔΓs=0.0657±0.0043(stat.)±0.0037(syst.)ps-1Γs=0.6703±0.0014(stat.)±0.0018(syst.)ps-1Results
for ϕs and Δ Γ s are also presented as 68% confidence
level contours in the ϕs–Δ Γ s plane. Furthermore the
transversity amplitudes and corresponding strong phases are
measured. ϕs and Δ Γ s measurements are in agreement with
the Standard Model predictions.},
Doi = {10.1140/epjc/s10052-021-09011-0},
Key = {fds365407}
}
@article{fds321183,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of the CP-violating phase ϕsand the
Bs0meson decay width difference with
Bs0→ J/ψϕ decays in
ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)147},
Abstract = {A measurement of the Bs0decay parameters in the Bs0→
J/ψϕ channel using an integrated luminosity of 14.3
fb−1collected by the ATLAS detector from 8 TeV pp
collisions at the LHC is presented. The measured parameters
include the CP -violating phase ϕs, the decay width Γs and
the width difference between the mass eigenstates ΔΓs. The
values measured for the physical parameters are
statistically combined with those from 4.9 fb−1of 7 TeV
data, leading to the following: Φs = -0.090 ± 0.078
(stat.) ± (syst.) rad Δ Γs = 0.085 ± 0.011 (stat.) ±
0.007 (syst.) Ps-1 Δ Γs = 0.675 ± 0.003 (stat.) ± 0.03
(syst.) Ps-1 In the analysis the parameter ΔΓs is
constrained to be positive. Results for ϕs and ΔΓs are
also presented as 68% and 95% likelihood contours in the
ϕs-ΔΓs plane. Also measured in this decay channel are the
transversity amplitudes and corresponding strong phases. All
measurements are in agreement with the Standard Model
predictions.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP08(2016)147},
Key = {fds321183}
}
@article{fds308839,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Culbertson, R and Dagenhart, D and Daniels, T and Jongh, FD and dell'Agnello, S and dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incadela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh,
SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips,
TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni,
A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt,
MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill,
A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok,
K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima,
R and Takikawa, K and Tanaka, M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko,
M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and Vejcik, S and Velev, G and Vidal, R and Vilar,
R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and Wester,
WC and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh,
GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of the CP-violation parameter sin(2β) in
Bd0/B̄d0 →
J/ψKS0 decays},
Journal = {Physical Review Letters},
Volume = {81},
Number = {25},
Pages = {5513-5518},
Year = {1998},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.5513},
Abstract = {We present a measurement of the time-dependent asymmetry in
the rate for B̄d0 versus Bd0 decays to J/ψ KS0. A nonzero
asymmetry would be an indication of CP violation, and within
the standard model this may be used to measure the
CP-violation parameter sin(2β). A total of 198 ± 17
Bd0/B̄d0 decays were observed in pp̄ collisions at √s =
1.8 TeV by the CDF detector at the Fermilab Tevatron. Bd0
and B̄d0 are distinguished by a technique based on charge
correlations from hadronization of the b quark. Our analysis
results in sin(2β) = 1.8 ± 1.1(stat) ±
0.3(syst).},
Doi = {10.1103/PhysRevLett.81.5513},
Key = {fds308839}
}
@article{fds308326,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and d'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucà, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of the cross section for direct-photon
production in association with a heavy quark in pp[over ¯]
collisions at sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {111},
Number = {4},
Pages = {042003},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.111.042003},
Abstract = {We report on a measurement of the cross section for
direct-photon production in association with a heavy quark
using the full data set of sqrt[s]=1.96 TeV
proton-antiproton collisions corresponding to 9.1 fb-1
of integrated luminosity collected by the CDF II detector at
the Fermilab Tevatron. The measurements are performed as a
function of the photon transverse momentum, covering a
photon transverse momentum between 30 and 300 GeV, photon
rapidities |yγ|<1.0, a heavy-quark-jet transverse momentum
pTjet>20 GeV, and jet rapidities |yjet|<1.5. The
results are compared with several theoretical
predictions.},
Doi = {10.1103/physrevlett.111.042003},
Key = {fds308326}
}
@article{fds308701,
Author = {Acosta, and D, and others},
Title = {Measurement of the cross section for prompt diphoton
production in p anti-p collisions at sqrt[s]=1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {95},
Number = {2},
Pages = {022003},
Year = {2005},
url = {http://dx.doi.org/10.1103/physrevlett.95.022003},
Abstract = {http://arxiv.org/abs/hep-ex/0412050},
Doi = {10.1103/physrevlett.95.022003},
Key = {fds308701}
}
@article{fds308429,
Author = {Aaltonen, TEA},
Title = {Measurement of the Cross Section for Prompt Isolated
Diphoton Production in $p\overline{p}$ Collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {10},
Pages = {102003},
Publisher = {American Physical Society},
Year = {2011},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.102003},
Abstract = {This Letter reports a measurement of the cross section of
prompt isolated photon pair production in pp collisions at a
total energy square root(s)=1.96 TeV using data of
5.36 fb(-1) integrated luminosity collected with the
CDF II detector at the Fermilab Tevatron. The measured cross
section, differential in basic kinematic variables, is
compared with three perturbative QCD predictions, a leading
order parton shower calculation and two next-to-leading
order calculations. The next-to-leading order calculations
reproduce most aspects of the data. By including photon
radiation from quarks before and after hard scattering, the
parton shower prediction becomes competitive with the
next-to-leading order predictions.},
Doi = {10.1103/PhysRevLett.107.102003},
Key = {fds308429}
}
@article{fds308339,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov,
A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Riddick, T and Rimondi,
F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani,
M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu,
V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song,
H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of the cross section for prompt isolated
diphoton production using the full CDF run II data
sample.},
Journal = {Physical review letters},
Volume = {110},
Number = {10},
Pages = {101801},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.110.101801},
Abstract = {This Letter reports a measurement of the cross section for
producing pairs of central prompt isolated photons in
proton-antiproton collisions at a total energy sqrt[s] =
1.96 TeV using data corresponding to 9.5 fb(-1) integrated
luminosity collected with the CDF II detector at the
Fermilab Tevatron. The measured differential cross section
is compared to three calculations derived from the theory of
strong interactions. These include a prediction based on a
leading order matrix element calculation merged with a
parton shower model, a next-to-leading order calculation,
and a next-to-next-to-leading order calculation. The first
and last calculations reproduce most aspects of the data,
thus showing the importance of higher-order contributions
for understanding the theory of strong interaction and
improving measurements of the Higgs boson and searches for
new phenomena in diphoton final states.},
Doi = {10.1103/physrevlett.110.101801},
Key = {fds308339}
}
@article{fds308719,
Author = {Acosta, and D, and others},
Title = {Measurement of the cross section for t anti-t production in
p anti-p collisions using the kinematics of lepton + jets
events},
Journal = {Phys. Rev.},
Volume = {D72},
Number = {5},
Pages = {052003},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.72.052003},
Abstract = {http://arxiv.org/abs/hep-ex/0504053},
Doi = {10.1103/PhysRevD.72.052003},
Key = {fds308719}
}
@article{fds336458,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
Title = {Measurement of the cross section for W-boson production in
association with jets in pp̄ collisions at
s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {77},
Number = {1},
Year = {2008},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.77.011108},
Abstract = {We present a measurement of the cross section for W-boson
production in association with jets in pp̄ collisions at
s=1.96TeV. The analysis uses a data sample corresponding to
an integrated luminosity of 320pb-1 collected with the CDF
II detector. W bosons are identified in their electron decay
channel and jets are reconstructed using a cone algorithm.
For each W+≥n-jet sample (n=1-4) we measure the
differential cross section dσ(pp̄→W+≥
n-jet)/dETnth-jet×B(W→eν) with respect to the transverse
energy ET of the nth-highest ET jet above 20GeV, and the
total cross section σ(pp̄→W+≥n-jet;ETnth-jet>25GeV)×B(W→eν),
for a restricted W→eν decay phase space. The cross
sections, corrected for all detector effects, can be
directly compared to particle level W+jet(s) predictions. We
present here comparisons to leading order and
next-to-leading order predictions. © 2008 The American
Physical Society.},
Doi = {10.1103/PhysRevD.77.011108},
Key = {fds336458}
}
@article{fds321354,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurement of the cross section of high transverse momentum
Z→bb¯ production in proton–proton collisions at √s=8
TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {738},
Pages = {25-43},
Publisher = {Elsevier BV},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2014.09.020},
Abstract = {This Letter reports the observation of a high transverse
momentum Z→bb¯ signal in proton–proton collisions at
s=8 TeV and the measurement of its production cross section.
The data analysed were collected in 2012 with the ATLAS
detector at the LHC and correspond to an integrated
luminosity of 19.5 fb−1. The Z→bb¯ decay is
reconstructed from a pair of b-tagged jets, clustered with
the anti-kt jet algorithm with R=0.4, that have low angular
separation and form a dijet with pT>200 GeV. The signal
yield is extracted from a fit to the dijet invariant mass
distribution, with the dominant, multi-jet background mass
shape estimated by employing a fully data-driven technique
that reduces the dependence of the analysis on simulation.
The fiducial cross section is determined to be
σZ→bb¯fid=2.02±0.20 (stat.) ±0.25 (syst.)±0.06
(lumi.) pb=2.02 ±0.33 pb, in good agreement with
next-to-leading-order theoretical predictions.},
Doi = {10.1016/j.physletb.2014.09.020},
Key = {fds321354}
}
@article{fds321315,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurement of the cross-section of high transverse momentum
vector bosons reconstructed as single jets and studies of
jet substructure in pp collisions at √s = 7 TeV with the
ATLAS detector},
Journal = {New Journal of Physics},
Volume = {16},
Number = {11},
Pages = {113013-113013},
Publisher = {IOP Publishing},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1088/1367-2630/16/11/113013},
Abstract = {This paper presents a measurement of the cross-section for
high transverse momentum W and Z bosons produced in pp
collisions and decaying to all-hadronic final states. The
data used in the analysis were recorded by the ATLAS
detector at the CERN Large Hadron Collider at a
centre-of-mass energy of and correspond to an integrated
luminosity of . The measurement is performed by
reconstructing the boosted W or Z bosons in single jets. The
reconstructed jet mass is used to identify the W and Z
bosons, and a jet substructure method based on energy
cluster information in the jet centre-of-mass frame is used
to suppress the large multi-jet background. The
cross-section for events with a hadronically decaying W or Z
boson, with transverse momentum and pseudorapidity , is
measured to be pb and is compared to next-to-leading-order
calculations. The selected events are further used to study
jet grooming techniques.},
Doi = {10.1088/1367-2630/16/11/113013},
Key = {fds321315}
}
@article{fds375893,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Measurement of the cross-sections of the electroweak and
total production of a Zγ pair in association with two jets
in pp collisions at s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {846},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138222},
Abstract = {This Letter presents the measurement of the fiducial and
differential cross-sections of the electroweak production of
a Zγ pair in association with two jets. The analysis uses
140 fb−1 of LHC proton–proton collision data taken at
s=13 TeV recorded by the ATLAS detector during the years
2015–2018. Events with a Z boson candidate decaying into
either an e+e− or μ+μ− pair, a photon and two jets are
selected. The electroweak component is extracted by
requiring a large dijet invariant mass and by using the
information about the centrality of the system and is
measured with an observed and expected significance well
above five standard deviations. The fiducial pp→Zγjj
cross-section for the electroweak production is measured to
be 3.6 ± 0.5 fb. The total fiducial cross-section that also
includes contributions where the jets arise from strong
interactions is measured to be 16.8−1.8+2.0 fb. The
results are consistent with the Standard Model predictions.
Differential cross-sections are also measured using the same
events and are compared with parton-shower Monte Carlo
simulations. Good agreement is observed between data and
predictions.},
Doi = {10.1016/j.physletb.2023.138222},
Key = {fds375893}
}
@article{fds308796,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den
Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer,
E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and de Jongh, F and dell'Agnello, S and dell'Orso,
M},
Title = {Measurement of the decay amplitudes of B0 →
J/ψK*0 and Bs0 → J/ψφ
decays},
Journal = {Physical Review Letters},
Volume = {85},
Number = {22},
Pages = {4668-4673},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.85.4668},
Abstract = {A full angular analysis of both the B0 and Bs0 decay modes
was carried out. For this analysis, the B0 → J/ψK*0 and
Bs0 → J/ψφ decays were reconstructed. The obtained data
were analyzed in detail.},
Doi = {10.1103/PhysRevLett.85.4668},
Key = {fds308796}
}
@article{fds308409,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of the difference in CP-violating asymmetries in
D(0)→K(+)K(-) and D(0)→π(+)π(-) decays at
CDF.},
Journal = {Physical review letters},
Volume = {109},
Number = {11},
Pages = {111801},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.109.111801},
Abstract = {We report a measurement of the difference (ΔA(CP)) between
time-integrated CP-violating asymmetries in D(0)→K(+)K(-)
and D(0)→π(+)π(-) decays reconstructed in the full data
set of proton-antiproton collisions collected by the
Collider Detector at Fermilab, corresponding to
9.7 fb(-1) of integrated luminosity. The strong decay
D(*+)→D(0)π(+) is used to identify the charm meson at
production as D(0) or D[over ¯](0). We measure
ΔA(CP)=[-0.62±0.21(stat)±0.10(syst)]%, which differs from
zero by 2.7 Gaussian standard deviations. This result
supports similar evidence for CP violation in charm-quark
decays obtained in proton-proton collisions.},
Doi = {10.1103/physrevlett.109.111801},
Key = {fds308409}
}
@article{fds308327,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Measurement of the differential cross section
dσ/d(cosθ(t)) for Top-Quark Pair Production in pp
Collisions at sqrt[s] = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {111},
Number = {18},
Pages = {182002},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.111.182002},
Abstract = {We report a measurement of the differential cross section
dσ/d(cosθ(t)) for top-quark pair production as a function
of the top-quark production angle in proton-antiproton
collisions at sqrt[s] = 1.96 TeV. This measurement is
performed using data collected with the CDF II detector at
the Tevatron, corresponding to an integrated luminosity of
9.4 fb(-1). We employ the Legendre polynomials to
characterize the shape of the differential cross section at
the parton level. The observed Legendre coefficients are in
good agreement with the prediction of the
next-to-leading-order standard-model calculation, with the
exception of an excess linear-term coefficient a(1) = 0.40
± 0.12, compared to the standard-model prediction of
a(1)=0.15(-0.03)(+0.07).},
Doi = {10.1103/physrevlett.111.182002},
Key = {fds308327}
}
@article{fds308305,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Measurement of the differential cross-section of B+ meson
production in pp collisions at √s = 7 TeV at
ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {10},
Pages = {1-37},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP10(2013)042},
Abstract = {The production cross-section of B+ mesons is measured as a
function of transverse momentum pT and rapidity y in
proton-proton collisions at centre-of-mass energy √s = 7
TeV, using 2.4 fb-1 of data recorded with the ATLAS detector
at the Large Hadron Collider. The differential production
cross-sections, determined in the range 9 GeV < pT < 120 GeV
and |y| < 2:25, are compared to next-to-leading-order
theoretical predictions. Copyright CERN.},
Doi = {10.1007/JHEP10(2013)042},
Key = {fds308305}
}
@article{fds323674,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
J},
Title = {Measurement of the differential cross-sections of prompt and
non-prompt production of [Formula: see text] and [Formula:
see text] in pp collisions at [Formula: see text] and
8 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {283},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4050-8},
Abstract = {The production rates of prompt and non-prompt [Formula: see
text] and [Formula: see text] mesons in their dimuon decay
modes are measured using 2.1 and 11.4 fb[Formula: see text]
of data collected with the ATLAS experiment at the Large
Hadron Collider, in proton-proton collisions at [Formula:
see text] and 8 respectively. Production cross-sections for
prompt as well as non-prompt sources, ratios of [Formula:
see text] to [Formula: see text] production, and the
fractions of non-prompt production for [Formula: see text]
and [Formula: see text] are measured as a function of meson
transverse momentum and rapidity. The measurements are
compared to theoretical predictions.},
Doi = {10.1140/epjc/s10052-016-4050-8},
Key = {fds323674}
}
@article{fds308794,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti,
A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandi, A and Brink, SVD and Bromberg, C and Brozovic,
M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell,
M and Caner, A and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang,
PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Ciobanu,
CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli,
M and Costanzo, D and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and Dejongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent,
PF and Devlin, T and Dittmann, JR and Donau, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Fiori,
I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer,
S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold,
M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos,
K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Kara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Herndon, M and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, MJ and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and Lecompte, T and IV, AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer,
N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti, P and McFarland,
KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore,
E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman, J and Nahn, S and Nakada,
H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti,
R and Papadimitriou, V and Pappas, SP and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom,
L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos,
F and Punzi, G and Ragan, K and Rakitine, A and Reher, D and Reichold, A and Riegler, W and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki,
T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton,
P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa, F and Valls, J and III, SV and Velev, G and Vidal, R and Vilar, R and Volobouev,
I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Waters,
D and Watts, T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of the differential dijet mass cross section in
pp̄ collisions at √s=1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {61},
Number = {9},
Pages = {1-6},
Year = {2000},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.61.091101},
Abstract = {We present a measurement of the cross section for production
of two or more jets as a function of dijet mass, based on an
integrated luminosity of 86 pb-1 collected with the Collider
Detector at Fermilab. Our dijet mass spectrum is described
within errors by next-to-leading order QCD predictions using
CTEQ4HJ parton distributions, and is in good agreement with
a similar measurement from the DØ experiment. ©2000 the
American Physical Society.},
Doi = {10.1103/PhysRevD.61.091101},
Key = {fds308794}
}
@article{fds308669,
Author = {Abulencia, and A, and others},
Title = {Measurement of the dipion mass spectrum in X(3872) --> J/psi
pi+ pi- decays},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {10},
Pages = {102002},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.102002},
Abstract = {We measure the dipion mass spectrum in X(3872) --> J/psi
pi++ pi+- decays using 360 pb-1 of p anti-p collisions at
s**(1/2) = 1.96 TeV collected with the CDF II detector. The
spectrum is fit with predictions for odd C-parity (3S_1,
1P_1, and 3D_J) charmonia decaying to J/psi pi++ pi+-, as
well as even C-parity states in which the pi+ons are from
rho0 decay. The latter case also encompasses exotic
interpretations, such as D0 D-bar*0 molecule. Only the 3S_1
and J/psi rho hypotheses are compatible with our data. Since
3S_1 is untenable on other grounds, decay via J/psi rho is
favored, which implies C = +1 for the X(3872). Models for
different J/psi-rho angular momenta L are considered.
Flexibility in the models, especially the introduction of
rho-omega interference, enable good descriptions of our data
for both L = 0 and 1.},
Doi = {10.1103/physrevlett.96.102002},
Key = {fds308669}
}
@article{fds308299,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Measurement of the distributions of event-by-event flow
harmonics in lead-lead collisions at √SNN =
2.76 TeV with the ATLAS detector at the LHC},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {11},
Publisher = {Springer Nature},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2013)183},
Abstract = {The distributions of event-by-event harmonic flow
coefficients υn for n = 2-4 are measured in √sNN =
2.76TeV Pb+Pb collisions using the ATLAS detector at the
LHC. The measurements are performed using charged particles
with transverse momentum pT > 0.5GeV and in the
pseudorapidity range |η| < 2.5 in a dataset of
approximately 7 μb-1 recorded in 2010. The shapes of the
υn distributions suggest that the associated flow vectors
are described by a two-dimensional Gaussian function in
central collisions for υ2 and over most of the measured
centrality range for υ3 and υ4. Significant deviations
from this function are observed for υ2 in mid-central and
peripheral collisions, and a small deviation is observed for
υ3 in mid-central collisions. In order to be sensitive to
these deviations, it is shown that the commonly used
multi-particle cumulants, involving four particles or more,
need to be measured with a precision better than a few
percent. The υn distributions are also measured
independently for charged particles with 0.5 < pT < 1 GeV
and pT > 1 GeV. When these distributions are rescaled to the
same mean values, the adjusted shapes are found to be nearly
the same for these two pT ranges. The υn distributions are
compared with the eccentricity distributions from two models
for the initial collision geometry: a Glauber model and a
model that includes corrections to the initial geometry due
to gluon saturation effects. Both models fail to describe
the experimental data consistently over most of the measured
centrality range. Copyright CERN.},
Doi = {10.1007/JHEP11(2013)183},
Key = {fds308299}
}
@article{fds321175,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Measurement of the double-differential high-mass Drell-Yan
cross section in pp collisions at √s = 8 TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)009},
Abstract = {This paper presents a measurement of the double-differential
cross section for the Drell-Yan Z/γ∗ → ℓ+ℓ− and
photon-induced γγ → ℓ+ℓ− processes where ℓ is an
electron or muon. The measurement is performed for invariant
masses of the lepton pairs, mℓℓ, between 116 GeV and
1500 GeV using a sample of 20.3 fb−1 of pp collisions data
at centre-of-mass energy of s=8 TeV collected by the ATLAS
detector at the LHC in 2012. The data are presented double
differentially in invariant mass and absolute dilepton
rapidity as well as in invariant mass and absolute
pseudorapidity separation of the lepton pair. The
single-differential cross section as a function of mℓℓ
is also reported. The electron and muon channel measurements
are combined and a total experimental precision of better
than 1% is achieved at low mℓℓ. A comparison to
next-to-next-to-leading order perturbative QCD predictions
using several recent parton distribution functions and
including next-to-leading order electroweak effects
indicates the potential of the data to constrain parton
distribution functions. In particular, a large impact of the
data on the photon PDF is demonstrated.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP08(2016)009},
Key = {fds321175}
}
@article{fds308280,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
VV and Dos Santos and SPA and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
Title = {Measurement of the electroweak production of dijets in
association with a Z-boson and distributions sensitive to
vector boson fusion in proton-proton collisions at √s= 8
TeV using the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {4},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP04(2014)031},
Doi = {10.1007/JHEP04(2014)031},
Key = {fds308280}
}
@article{fds365356,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari,
N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C},
Title = {Measurement of the energy asymmetry in tt¯ j production at
13 TeV with the ATLAS experiment and interpretation in the
SMEFT framework},
Journal = {European Physical Journal C},
Volume = {82},
Number = {4},
Year = {2022},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10101-w},
Abstract = {A measurement of the energy asymmetry in jet-associated
top-quark pair production is presented using 139fb-1 of data
collected by the ATLAS detector at the Large Hadron Collider
during pp collisions at s=13TeV. The observable measures the
different probability of top and antitop quarks to have the
higher energy as a function of the jet scattering angle with
respect to the beam axis. The energy asymmetry is measured
in the semileptonic tt¯ decay channel, and the hadronically
decaying top quark must have transverse momentum above
350GeV. The results are corrected for detector effects to
particle level in three bins of the scattering angle of the
associated jet. The measurement agrees with the SM
prediction at next-to-leading-order accuracy in quantum
chromodynamics in all three bins. In the bin with the
largest expected asymmetry, where the jet is emitted
perpendicular to the beam, the energy asymmetry is measured
to be - 0.043 ± 0.020 , in agreement with the SM prediction
of - 0.037 ± 0.003. Interpreting this result in the
framework of the Standard Model effective field theory
(SMEFT), it is shown that the energy asymmetry is sensitive
to the top-quark chirality in four-quark operators and is
therefore a valuable new observable in global SMEFT
fits.},
Doi = {10.1140/epjc/s10052-022-10101-w},
Key = {fds365356}
}
@article{fds365359,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Measurement of the energy response of the ATLAS calorimeter
to charged pions from W±→ τ±(→
π±ντ) ντ events in
Run 2 data},
Journal = {European Physical Journal C},
Volume = {82},
Number = {3},
Year = {2022},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10117-2},
Abstract = {The energy response of the ATLAS calorimeter is measured for
single charged pions with transverse momentum in the range
10 < pT< 300 GeV. The measurement is performed using 139 fb
- 1 of LHC proton–proton collision data at s=13 TeV taken
in Run 2 by the ATLAS detector. Charged pions originating
from τ-lepton decays are used to provide a sample of
high-pT isolated particles, where the composition is known,
to test an energy regime that has not previously been probed
by in situ single-particle measurements. The calorimeter
response to single-pions is observed to be overestimated by
∼ 2 % across a large part of the pT spectrum in the
central region and underestimated by ∼ 4 % in the endcaps
in the ATLAS simulation. The uncertainties in the
measurements are ≲ 1 % for 15 < pT< 185 GeV in the central
region. To investigate the source of the discrepancies, the
width of the distribution of the ratio of calorimeter energy
to track momentum, the energies per layer and response in
the hadronic calorimeter are also compared between data and
simulation.},
Doi = {10.1140/epjc/s10052-022-10117-2},
Key = {fds365359}
}
@article{fds321191,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Erbacher, R and Errede, S and Esham,
B},
Title = {Measurement of the forward-backward asymmetry in low-mass
bottom-quark pairs produced in proton-antiproton
collisions},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112003},
Abstract = {We report a measurement of the forward-backward asymmetry,
AFB, in bb pairs produced in proton-antiproton collisions
and identified by muons from semileptonic b-hadron decays.
The event sample is collected at a center-of-mass energy of
s=1.96 TeV with the CDF II detector and corresponds to 6.9
fb-1 of integrated luminosity. We obtain an integrated
asymmetry of AFB(bb)=(1.2±0.7)% at the particle level for
b-quark pairs with invariant mass, mbb, down to 40 GeV/c2
and measure the dependence of AFB(bb) on mbb. The results
are compatible with expectations from the standard
model.},
Doi = {10.1103/PhysRevD.93.112003},
Key = {fds321191}
}
@article{fds308449,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of the Forward-Backward Asymmetry in the
${B}\rightarrow{K}^{(*)}\mu^{+}\mu^{-}$ Decay and First
Observation of the ${B}_{s}^{0}$\rightarrow${}$\phi${}{$\mu${}}^{+}{$\mu${}}^{-}$
Decay},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {16},
Pages = {161801},
Publisher = {American Physical Society},
Year = {2011},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.161801},
Abstract = {We reconstruct the rare decays B(+)→K(+)μ(+0μ(-0,
B90)→K*(892)(0)μ(+)μ(-), and B(s)(0)→ϕ(1020)μ(+)μ(-)
in a data sample corresponding to 4.4 fb(-1) collected
in pp collisions at √[s]=1.96 TeV by the CDF II
detector at the Tevatron Collider. Using 121±16
B(+)→K(+)μ(+)μ(-) and 101±12 B(0)→K(*0)μ(+)μ(-)
decays we report the branching ratios. In addition, we
report the differential branching ratio and the muon
forward-backward asymmetry in the B(+) and B(0) decay modes,
and the K(*0) longitudinal polarization fraction in the B(0)
decay mode with respect to the squared dimuon mass. These
are consistent with the predictions, and most recent
determinations from other experiments and of comparable
accuracy. We also report the first observation of the
B(s)(0)→ϕμ(+)μ(-) decay and measure its branching ratio
BR(B(s)(0)→ϕμ(+)μ(-))=[1.44±0.33±0.46]×10(-6) using
27±6 signal events. This is currently the most rare B(s)(0)
decay observed.},
Doi = {10.1103/PhysRevLett.106.161801},
Key = {fds308449}
}
@article{fds314183,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the forward-backward asymmetry of electron
and muon pair-production in pp collisions at √s=7 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {9},
Pages = {1-43},
Publisher = {Springer Nature},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2015)049},
Abstract = {This paper presents measurements from the ATLAS experiment
of the forward-backward asymmetry in the reaction pp →
Z/γ* → l+l−, with l being electrons or muons, and the
extraction of the effective weak mixing angle. The results
are based on the full set of data collected in 2011 in pp
collisions at the LHC at (Formula presented.), corresponding
to an integrated luminosity of 4.8 fb−1. The measured
asymmetry values are found to be in agreement with the
corresponding Standard Model predictions. The combination of
the muon and electron channels yields a value of the
effective weak mixing angle of sin2θefflept = 0.2308 ±
0.0005(stat.) ± 0.0006(syst.) ± 0.0009(PDF), where the
first uncertainty corresponds to data statistics, the second
to systematic effects and the third to knowledge of the
parton density functions. This result agrees with the
current world average from the Particle Data Group
fit.},
Doi = {10.1007/JHEP09(2015)049},
Key = {fds314183}
}
@article{fds321192,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Erbacher, R and Errede, S and Esham,
B},
Title = {Measurement of the forward-backward asymmetry of top-quark
and antiquark pairs using the full CDF Run II data
set},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112005},
Abstract = {We measure the forward-backward asymmetry of the production
of top-quark and antiquark pairs in proton-antiproton
collisions at center-of-mass energy s=1.96 TeV using the
full data set collected by the Collider Detector at Fermilab
(CDF) in Tevatron Run II corresponding to an integrated
luminosity of 9.1 fb-1. The asymmetry is characterized by
the rapidity difference between top quarks and antiquarks
(Δy) and measured in the final state with two charged
leptons (electrons and muons). The inclusive asymmetry,
corrected to the entire phase space at parton level, is
measured to be AFBtt=0.12±0.13, consistent with the
expectations from the standard model (SM) and previous CDF
results in the final state with a single charged lepton. The
combination of the CDF measurements of the inclusive AFBtt
in both final states yields AFBtt=0.160±0.045, which is
consistent with the SM predictions. We also measure the
differential asymmetry as a function of Δy. A linear fit to
AFBtt(|Δy|), assuming zero asymmetry at Δy=0, yields a
slope of α=0.14±0.15, consistent with the SM prediction
and the previous CDF determination in the final state with a
single charged lepton. The combined slope of AFBtt(|Δy|) in
the two final states is α=0.227±0.057, which is 2.0σ
larger than the SM prediction.},
Doi = {10.1103/PhysRevD.93.112005},
Key = {fds321192}
}
@article{fds321373,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen,
D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy,
L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard,
PF},
Title = {Measurement of the forward-backward charge asymmetry from
W→ev production in pp̄ collisions at √s=1.96
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {5},
Pages = {1-9},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.051104},
Abstract = {We report a measurement of the forward-backward charge
asymmetry of electrons from W boson decays in pp̄
collisions at √s=1.96 TeV using a data sample of 170 pb-1
collected by the Collider Detector at Fermilab. The
asymmetry is measured as a function of electron rapidity and
transverse energy and provides new input on the momentum
fraction dependence of the u and d quark parton distribution
functions within the proton. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevD.71.051104},
Key = {fds321373}
}
@article{fds337970,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Copic, K and Cordelli, M and Cortiana, G and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson,
R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and Barbaro,
PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler,
A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori,
M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, RS and Lucchesi, D and Lueck,
J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou,
A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts,
K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn,
F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi,
G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle,
T and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shiraishi,
S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith,
JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B},
Title = {Measurement of the fraction of tt̄ production via
gluon-gluon fusion in pp̄ collisions at
s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {3},
Pages = {031101},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.031101},
Abstract = {We present a measurement of the ratio of the tt̄ production
cross section via gluon-gluon fusion to the total tt̄
production cross section in pp̄ collisions at s=1.96TeV at
the Tevatron. Using a data sample with an integrated
luminosity of 955pb-1 recorded by the CDF II detector at
Fermilab, we select events based on the tt̄ decay to
lepton+jets. Using an artificial neural network technique we
discriminate between tt̄ events produced via qq̄
annihilation and gg fusion, and find Gf=σ(gg→tt̄)/
σ(pp̄→tt̄)<0.33 at the 68% confidence level. This
result is combined with a previous measurement to obtain the
most stringent measurement of this quantity by CDF to date,
Gf=0.07-0.07+0.15. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevD.79.031101},
Key = {fds337970}
}
@article{fds308876,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg,
C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C},
Title = {Measurement of the gamma +D*+/- Cross Section in p-barp
Collisions at sqrt s=1.8 TeV.},
Journal = {Physical review letters},
Volume = {77},
Number = {25},
Pages = {5005-5010},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.77.5005},
Abstract = {We have measured the cross section of γ + D* ± production
in pp collisions at √ = 1.8 TeV using the Collider
Detector at Fermilab. In this kinematic region, the Compton
scattering process (gc → γ c) is expected to dominate and
thus provide a direct link to the charm quark density in the
proton. From the 45 ± 18 γ + D* ± candidates in a 16.4
pb− 1 data sample, we have determined the production cross
section to be 0.38 ± 0.15 ± (stat) ± 0.11(syst)nb for the
rapidity range | y(D* ±)| < 1.2 and | y (γ) | < 0.9, and
for the transverse momentum range pT(D* ±) > 6GeV/c and 16
< pT(γ) < 40 GeV/c. The measured cross section is compared
to a theoretical prediction. © 1996 The American Physical
Society.},
Doi = {10.1103/physrevlett.77.5005},
Key = {fds308876}
}
@article{fds308648,
Author = {Abulencia, and A, and others},
Title = {Measurement of the Helicity Fractions of W Bosons from Top
Quark Decays using Fully Reconstructed \boldmath${t\bar{t}}$
Events with CDF II},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {5},
Pages = {052001},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.052001},
Abstract = {We present a measurement of the fractions F0 and F+ of
longitudinally polarized and right-handed W bosons in
top-quark decays using data collected with the CDF II
detector. The data set used in the analysis corresponds to
an integrated luminosity of approximately 318 pb-1. We
select t[overline t] candidate events with one lepton, at
least four jets, and missing transverse energy. Our helicity
measurement uses the decay angle theta*, which is defined as
the angle between the momentum of the charged lepton in the
W boson rest frame and the W momentum in the top-quark rest
frame. The costheta* distribution in the data is determined
by full kinematic reconstruction of the t[overline t]
candidates. We find F0=0.85-0.22+0.15(stat)$\pm$0.06(syst)
and F+=0.05-0.05+0.11(stat)$\pm$0.03(syst), which is
consistent with the standard model prediction. We set an
upper limit on the fraction of right-handed W bosons of
F+},
Doi = {10.1103/PhysRevD.75.052001},
Key = {fds308648}
}
@article{fds308679,
Author = {collaboration, CDF},
Title = {Measurement of the Helicity of W Bosons in Top Quark
Decays},
Journal = {Phys.Rev.Lett.},
Volume = {84},
Number = {11},
Pages = {216-221},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.73.111103},
Abstract = {http://arXiv.org/ps/hep-ex/9909042},
Doi = {10.1103/PhysRevD.73.111103},
Key = {fds308679}
}
@article{fds331644,
Author = {Ukegawa, F and Valls, J and Vejcik, S and Velev, G and Vidal, R and Vilar,
R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl,
J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
BL},
Title = {Measurement of the helicity of W bosons in top quark
decays},
Journal = {Physical review letters},
Volume = {84},
Number = {2},
Pages = {216-221},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://arXiv.org/ps/hep-ex/9909042},
Abstract = {We use the transverse momentum spectrum of leptons in the
decay chain t-->bW with W-->lnu to measure the helicity of
the W bosons in the top quark rest frame. Our measurement
uses a t&tmacr; sample isolated in 106+/-4 pb(-1) of data
collected in p&pmacr; collisions at sqrt[s] = 1.8 TeV with
the CDF detector at the Fermilab Tevatron. Assuming a
standard V-A weak decay, we find that the fraction of W's
with zero helicity in the top rest frame is F0 = 0.91+/-0.
37(stat)+/-0.13(syst), consistent with the standard model
prediction of F0 = 0.70 for a top mass of 175
GeV/c(2).},
Doi = {10.1103/physrevlett.84.216},
Key = {fds331644}
}
@article{fds321338,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abidi, SH and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the Higgs boson mass from the H → γγ and
H → ZZ∗- 4ℓ channels inpp collisions at
center-of-mass energies of 7 and 8 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.90.052004},
Abstract = {An improved measurement of the mass of the Higgs boson is
derived from a combined fit to the reconstructed invariant
mass spectra of the decay channels H → γγ and H →
ZZ∗→ 4ℓ. The analysis uses the pp collision data
sample recorded by the ATLAS experiment at the CERN Large
Hadron Collider at center-of-mass energies of 7 TeV and 8
TeV, corresponding to an integrated luminosity of 25 fb-1.
The measured value of the Higgs boson mass is mH= 125.36 ±
0.37(stat) ± 0.18(syst) GeV. This result is based on
improved energy-scale calibrations for photons, electrons,
and muons as well as other analysis improvements, and
supersedes the previous result from ATLAS. Upper limits on
the total width of the Higgs boson are derived from fits to
the invariant mass spectra of the H → γγ and H →
ZZ∗→ 4ℓ decay channels.},
Doi = {10.1103/PhysRevD.90.052004},
Key = {fds321338}
}
@article{fds375915,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V},
Title = {Measurement of the Higgs boson mass in the
H → ZZ⁎ → 4ℓ decay channel using
139 fb−1 of s=13 TeV pp collisions recorded by
the ATLAS detector at the LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137880},
Abstract = {The mass of the Higgs boson is measured in the
H→ZZ⁎→4ℓ decay channel. The analysis uses
proton–proton collision data from the Large Hadron
Collider at a centre-of-mass energy of 13 TeV recorded by
the ATLAS detector between 2015 and 2018, corresponding to
an integrated luminosity of 139 fb−1. The measured value
of the Higgs boson mass is 124.99±0.18(stat.)±0.04(syst.)
GeV. In final states with muons, this measurement benefits
from an improved momentum-scale calibration relative to that
adopted in previous publications. The measurement also
employs an analytic model that takes into account the
invariant-mass resolution of the four-lepton system on a
per-event basis and the output of a deep neural network
discriminating signal from background events. This
measurement is combined with the corresponding measurement
using 7 and 8 TeV pp collision data, resulting in a Higgs
boson mass of 124.94±0.17(stat.)±0.03(syst.)
GeV.},
Doi = {10.1016/j.physletb.2023.137880},
Key = {fds375915}
}
@article{fds375884,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Measurement of the Higgs boson mass with H → γγ
decays in 140 fb−1 of s=13 TeV pp collisions
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {847},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138315},
Abstract = {The mass of the Higgs boson is measured in the H→γγ
decay channel, exploiting the high resolution of the
invariant mass of photon pairs reconstructed from the decays
of Higgs bosons produced in proton–proton collisions at a
centre-of-mass energy s=13 TeV. The dataset was collected
between 2015 and 2018 by the ATLAS detector at the Large
Hadron Collider, and corresponds to an integrated luminosity
of 140 fb−1. The measured value of the Higgs boson mass is
125.17±0.11(stat.)±0.09(syst.) GeV and is based on an
improved energy scale calibration for photons, whose impact
on the measurement is about four times smaller than in the
previous publication. A combination with the corresponding
measurement using 7 and 8 TeV pp collision ATLAS data
results in a Higgs boson mass measurement of
125.22±0.11(stat.)±0.09(syst.) GeV. With an uncertainty of
1.1 per mille, this is currently the most precise
measurement of the mass of the Higgs boson from a single
decay channel.},
Doi = {10.1016/j.physletb.2023.138315},
Key = {fds375884}
}
@article{fds308362,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Measurement of the high-mass Drell–Yan differential
cross-section in pp collisions at √s=7TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {725},
Number = {4-5},
Pages = {223-242},
Publisher = {Elsevier BV},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2013.07.049},
Abstract = {This Letter reports a measurement of the high-mass
Drell–Yan differential cross-section in proton–proton
collisions at a centre-of-mass energy of 7 TeV at the LHC.
Based on an integrated luminosity of 4.9 fb−1, the
differential cross-section in the Z/γ⁎→e+e− channel
is measured with the ATLAS detector as a function of the
invariant mass, mee, in the range 116 <mee <1500 GeV, for a
fiducial region in which both the electron and the positron
have transverse momentum pT >25 GeV and pseudorapidity |η|
<2.5. A comparison is made to various event generators and
to the predictions of perturbative QCD calculations at
next-to-next-to-leading order.},
Doi = {10.1016/j.physletb.2013.07.049},
Key = {fds308362}
}
@article{fds375879,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye,
T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja,
S and Ai, X and Aielli, G and Aikot, A and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Cardoso, MA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler,
A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Dos Santos,
SPA and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA},
Title = {Measurement of the H→ γγ and H→ ZZ∗→ 4
ℓ cross-sections in pp collisions at √s=13.6 TeV with
the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {84},
Number = {1},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-12130-5},
Abstract = {The inclusive Higgs boson production cross-section is
measured in the di-photon and the ZZ∗→ 4 ℓ decay
channels using 31.4 and 29.0 fb - 1 of pp collision data
respectively, collected with the ATLAS detector at a
centre-of-mass energy of s=13.6 TeV . To reduce the model
dependence, the measurement in each channel is restricted to
a particle-level phase space that closely matches the
channel’s detector-level kinematic selection, and it is
corrected for detector effects. These measured fiducial
cross-sections are σfid,γγ= 76-13+14 fb, and σfid,4ℓ=
2.80±0.74 fb, in agreement with the corresponding Standard
Model predictions of 67.6 ± 3.7 fb and 3.67 ± 0.19 fb.
Assuming Standard Model acceptances and branching fractions
for the two channels, the fiducial measurements are
extrapolated to the full phase space yielding total
cross-sections of σ(pp→H)=67-11+12 pb and 46 ± 12 pb at
13.6 TeV from the di-photon and ZZ∗→ 4 ℓ measurements
respectively. The two measurements are combined into a total
cross-section measurement of σ(pp→ H) = 58.2 ± 8.7 pb,
to be compared with the Standard Model prediction of
σ(pp→ H) SM= 59.9 ± 2.6 pb.},
Doi = {10.1140/epjc/s10052-023-12130-5},
Key = {fds375879}
}
@article{fds375921,
Author = {Jackson, P and Oliver, JL and Petridis, A and Qureshi, A and Sharma, AS and White, MJ and Cairo, VMM and Jain, V and Swift, SP and Gingrich, DM and Pinfold, JL and Sun, X and Wang, H and Cakir, O and Yildiz, HD and Kuday,
S and Turk Cakir and I and Sultansoy, S and Berger, N and Costanza, F and Dartsi, O and Delmastro, M and Di Ciaccio and L and Falke, PJ and Falke, S and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Kivernyk, O and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo
Martinez, N and Raspopov, S and Sauvan, E and Smart, BH and Todorova-Nova, S and Vallier, A and Wingerter-Seez, I and Abulaiti,
Y and Benjamin, DP and Chekanov, S and Hopkins, WH and LeCompte, T and Liu,
BX and Love, J and Malon, D and Metcalfe, J and Paramonov, A and Proudfoot,
J and Ryu, S and Stanek, RW and Van Gemmeren and P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Delitzsch, CM and Johns, KA and Jones, S and Lampl, W and LeBlanc, M and Leone, R and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and De, K and Farbin, A and Griffiths, J and Hadavand, HK and Heelan, L and Little,
JD and Ozturk, N and Usai, G and White, A and Bellos, P and Fassouliotis,
D and Gkialas, I and Kourkoumelis, C and Papageorgiou, K and Tsirintanis, N and Alexopoulos, T and Bakalis, C and Benekos, N and Gazis, EN and Gkountoumis, P and Koulouris, A and Maltezos, S and Moschovakos, P and Panagoulias, I and Zacharis, G and Andeen, T and Narayan, R and Nikiforou, N and Onyisi, PUE and Potti,
H},
Title = {Measurement of the inclusive Formula Presented production
cross section in the lepton+jets channel in pp collisions at
Formula Presented with the ATLAS detector using support
vector machines},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032014},
Abstract = {A measurement of the top quark pair-production cross section
in the lepton + jets decay channel is presented. It is based
on 4.6 fb - 1 of s = 7 TeV p p collision data collected
during 2011 by the ATLAS experiment at the CERN Large Hadron
Collider. A three-class, multidimensional event classifier
based on support vector machines is used to differentiate t
t ¯ events from backgrounds. The t t ¯ production cross
section is found to be σ t t ¯ = 168.5 ± 0.7 ( stat ) -
5.9 + 6.2 ( syst ) - 3.2 + 3.4 ( lumi ) pb . The result is
consistent with the Standard Model prediction based on QCD
calculations at next-to-next-to-leading order.},
Doi = {10.1103/PhysRevD.108.032014},
Key = {fds375921}
}
@article{fds308571,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the inclusive isolated prompt photon cross
section in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
collisions at $\sqrt{s}=1.96\,\,TeV$ using the CDF
detector},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {11},
Pages = {111106},
Publisher = {American Physical Society},
Year = {2009},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.80.111106},
Abstract = {A measurement of the cross section for the inclusive
production of isolated photons by the CDF experiment at the
Fermilab Tevatron collider is presented. The measurement
covers the pseudorapidity region $|\eta\gamma|30$ GeV
and is based on 2.5 fb-1 of integrated luminosity. The
sample is almost a factor of 7 larger than those used for
recent published results and extends the $E_T^\gamma$
coverage by 100 GeV. The result agrees with next-to-leading
order perturbative QCD calculations within uncertainties
over the range $50},
Doi = {10.1103/PhysRevD.80.111106},
Key = {fds308571}
}
@article{fds321176,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
H},
Title = {Measurement of the inclusive isolated prompt photon cross
section in pp collisions at s=8TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)005},
Abstract = {Abstract: A measurement of the cross section for the
inclusive production of isolated prompt photons in
proton-proton collisions at a centre-of-mass energy of s=8
TeV is presented. The measurement covers the pseudorapidity
ranges |ηγ | < 1.37 and 1.56 ≤ |ηγ | < 2.37 in the
transverse energy range 25 < ETγ < 1500 GeV. The results
are based on an integrated luminosity of 20.2 fb−1,
recorded by the ATLAS detector at the LHC. Photon candidates
are identified by combining information from the
calorimeters and the inner tracker. The background is
subtracted using a data-driven technique, based on the
observed calorimeter shower-shape variables and the
deposition of hadronic energy in a narrow cone around the
photon candidate. The measured cross sections are compared
with leading-order and next-to-leading order perturbative
QCD calculations and are found to be in a good agreement
over ten orders of magnitude.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP08(2016)005},
Key = {fds321176}
}
@article{fds308283,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Measurement of the inclusive isolated prompt photons cross
section in pp collisions at √s =7 TeV with the ATLAS
detector using 4.6 fb-1},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.89.052004},
Abstract = {A measurement of the cross section for the production of
isolated prompt photons in pp collisions at a center-of-mass
energy √s=7 TeV is presented. The results are based on an
integrated luminosity of 4.6 fb-1 collected with the ATLAS
detector at the LHC. The cross section is measured as a
function of photon pseudorapidity ηγ and transverse energy
ETγ in the kinematic range 100≤ETγ<1000 GeV and in the
regions |ηγ|<1.37 and 1.52≤|ηγ|<2.37. The results are
compared to leading-order parton-shower Monte Carlo models
and next-to-leading-order perturbative QCD calculations.
Next-to-leading-order perturbative QCD calculations agree
well with the measured cross sections as a function of ETγ
and ηγ.},
Doi = {10.1103/PhysRevD.89.052004},
Key = {fds308283}
}
@article{fds308680,
Author = {Abulencia, and A, and others},
Title = {Measurement of the inclusive jet cross section in ppbar
Interactions at sqrt{s}=1.96 TeV Using a Cone-based Jet
Algorithm},
Journal = {Phys. Rev.},
Volume = {D74},
Number = {7},
Pages = {071103},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.74.071103},
Abstract = {We present a measurement of the inclusive jet cross section
in ppbar interactions at sqrt{s}=1.96 TeV using 385 pb^{-1}
of data collected with the CDF II detector at the Fermilab
Tevatron. The results are obtained using an improved
cone-based jet algorithm (Midpoint). The data cover the jet
transverse momentum range from 61 to 620 GeV/c, extending
the reach by almost 150 GeV/c compared with previous
measurements at the Tevatron. The results are in good
agreement with next-to-leading order perturbative QCD
predictions using the CTEQ6.1M parton distribution
functions.},
Doi = {10.1103/PhysRevD.74.071103},
Key = {fds308680}
}
@article{fds308668,
Author = {Abulencia, and A, and others},
Title = {Measurement of the inclusive jet cross section using the
k(t) algorithm in p anti-p collisions at $\sqrt{s}=$ 1.96-
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {12},
Pages = {122001},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.122001},
Abstract = {We report on a measurement of the inclusive jet production
cross section in p anti-p collisions at s**(1/2) = 1.96 TeV
using data collected with the upgraded Collider Detector at
Fermilab in Run II (CDF II) corresponding to an integrated
luminosity of 385 pb-1. Jets are reconstructed using the K_T
algorithm. The measurement is carried out for jets with
rapidity $0.1},
Doi = {10.1103/physrevlett.96.122001},
Key = {fds308668}
}
@article{fds308646,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
MA},
Title = {Measurement of the inclusive jet cross section using the kT
algorithm in pp̄ collisions at s=1.96TeV with the CDF II
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {75},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2007},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.75.092006},
Abstract = {We report on measurements of the inclusive jet production
cross section as a function of the jet transverse momentum
in pp̄ collisions at s=1.96TeV, using the kT algorithm and
a data sample corresponding to 1.0fb-1 collected with the
Collider Detector at Fermilab in run II. The measurements
are carried out in five different jet rapidity regions with
|yjet|<2.1 and transverse momentum in the range
54<pTjet<700GeV/c. Next-to-leading order perturbative QCD
predictions are in good agreement with the measured cross
sections. © 2007 The American Physical Society.},
Doi = {10.1103/PhysRevD.75.092006},
Key = {fds308646}
}
@article{fds308321,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, KM and Blair,
RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A},
Title = {Measurement of the inclusive jet cross-section in pp
collisions at [Formula: see text] and comparison to the
inclusive jet cross-section at [Formula: see text] using the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {8},
Pages = {2509},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2509-4},
Abstract = {The inclusive jet cross-section has been measured in
proton-proton collisions at [Formula: see text] in a dataset
corresponding to an integrated luminosity of [Formula: see
text] collected with the ATLAS detector at the Large Hadron
Collider in 2011. Jets are identified using the
anti-<i>k</i><sub><i>t</i></sub> algorithm with two radius
parameters of 0.4 and 0.6. The inclusive jet
double-differential cross-section is presented as a function
of the jet transverse momentum <i>p</i><sub>T</sub> and jet
rapidity <i>y</i>, covering a range of 20≤<i>p</i><sub>T</sub><430 GeV
and |<i>y</i>|<4.4. The ratio of the cross-section to the
inclusive jet cross-section measurement at [Formula: see
text], published by the ATLAS Collaboration, is calculated
as a function of both transverse momentum and the
dimensionless quantity [Formula: see text], in bins of jet
rapidity. The systematic uncertainties on the ratios are
significantly reduced due to the cancellation of correlated
uncertainties in the two measurements. Results are compared
to the prediction from next-to-leading order perturbative
QCD calculations corrected for non-perturbative effects, and
next-to-leading order Monte Carlo simulation. Furthermore,
the ATLAS jet cross-section measurements at [Formula: see
text] and [Formula: see text] are analysed within a
framework of next-to-leading order perturbative QCD
calculations to determine parton distribution functions of
the proton, taking into account the correlations between the
measurements.},
Doi = {10.1140/epjc/s10052-013-2509-4},
Key = {fds308321}
}
@article{fds321271,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the inclusive jet cross-section in
proton-proton collisions at √s=7 TeV using 4.5
fb−1 of data with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {2},
Pages = {1-54},
Publisher = {Springer Nature},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2015)153},
Abstract = {Abstract: The inclusive jet cross-section is measured in
proton-proton collisions at a centre-of-mass energy of 7 TeV
using a data set corresponding to an integrated luminosity
of 4.5 fb−1 collected with the ATLAS detector at the Large
Hadron Collider in 2011. Jets are identified using the
anti-kt algorithm with radius parameter values of 0.4 and
0.6. The double-differential cross-sections are presented as
a function of the jet transverse momentum and the jet
rapidity, covering jet transverse momenta from 100 GeV to 2
TeV. Next-to-leading-order QCD calculations corrected for
non-perturbative effects and electroweak effects, as well as
Monte Carlo simulations with next-to-leading-order matrix
elements interfaced to parton showering, are compared to the
measured cross-sections. A quantitative comparison of the
measured cross-sections to the QCD calculations using
several sets of parton distribution functions is
performed.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP02(2015)153},
Key = {fds321271}
}
@article{fds321343,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Henry, S and Herndon,
M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta,
A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra,
A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of the inclusive leptonic asymmetry in top-quark
pairs that decay to two charged leptons at
CDF.},
Journal = {Physical review letters},
Volume = {113},
Number = {4},
Pages = {042001},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.113.042001},
Abstract = {We measure the inclusive forward-backward asymmetry of the
charged-lepton pseudorapidities from top-quark pairs
produced in proton-antiproton collisions and decaying to
final states that contain two charged leptons (electrons or
muons). The data are collected with the Collider Detector at
Fermilab and correspond to an integrated luminosity of 9.1
fb(-1). We measure the leptonic forward-backward asymmetry,
A(FB)(ℓ), to be 0.072 ± 0.060 and the leptonic pair
forward-backward asymmetry, A(FB)(ℓℓ), to be 0.076 ±
0.082. The measured values can be compared with the standard
model predictions of A(FB)(ℓ) = 0.038 ± 0.003 and
A(FB)(ℓℓ) = 0.048 ± 0.004, respectively. Additionally,
we combine the A(FB)(ℓ) result with a previous
determination from a final state with a single lepton and
hadronic jets and obtain A(FB)(ℓ) = 0.090(-0.026)(+0.028).},
Doi = {10.1103/physrevlett.113.042001},
Key = {fds321343}
}
@article{fds321152,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
J and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M},
Title = {Measurement of the Inelastic Proton-Proton Cross Section at
sqrt[s]=13 TeV with the ATLAS Detector at the
LHC.},
Journal = {Phys Rev Lett},
Volume = {117},
Number = {18},
Pages = {182002},
Year = {2016},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevLett.117.182002},
Abstract = {This Letter presents a measurement of the inelastic
proton-proton cross section using 60 μb^{-1} of pp
collisions at a center-of-mass energy sqrt[s] of 13 TeV
with the ATLAS detector at the LHC. Inelastic interactions
are selected using rings of plastic scintillators in the
forward region (2.07<|η|<3.86) of the detector. A cross
section of 68.1±1.4 mb is measured in the fiducial
region ξ=M_{X}^{2}/s>10^{-6}, where M_{X} is the larger
invariant mass of the two hadronic systems separated by the
largest rapidity gap in the event. In this ξ range the
scintillators are highly efficient. For diffractive events
this corresponds to cases where at least one proton
dissociates to a system with M_{X}>13 GeV. The measured
cross section is compared with a range of theoretical
predictions. When extrapolated to the full phase space, a
cross section of 78.1±2.9 mb is measured, consistent
with the inelastic cross section increasing with
center-of-mass energy.},
Doi = {10.1103/PhysRevLett.117.182002},
Key = {fds321152}
}
@article{fds340915,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
L and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and DrollingerV, and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, V and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and HaywardH, and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and HoffmanK, D and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen,
D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
D},
Title = {Measurement of the J/ψ meson and b-hadron production cross
sections in pp̄ collisions at √s = 1960
GeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {3},
Pages = {032001-1-032001-26},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.032001},
Abstract = {We present a new measurement of the inclusive and
differential production cross sections of J/ψ mesons and b
hadrons in proton-antiproton collisions at √s = 1960 GeV.
The data correspond to an integrated luminosity of 39.7 pb-1
collected by the CDF run II detector. We find the integrated
cross section for inclusive J/ψ production for all
transverse momenta from 0 to 20 GeV/c in the rapidity range
|y| < 0.6 to be 4.08 ± 0.02(Stat)-0.33+0.36(syst) μb.
We separate the fraction of J/ψ events from the decay of
the long-lived b hadrons using the lifetime distribution in
all events with pT(J/ψ) > 1.25 GeV/c. We find the total
cross section for b hadrons, including both hadrons and
antihadrons, decaying to J/ψ with transverse momenta
greater than 1.25 GeV/c in the rapidity range |y(J/ψ)| <
0.6 is 0.330 ± 0.005(stat) -0.033+0.036(syst) μb. Using a
Monte Carlo simulation of the decay kinematics of b hadrons
to all final states containing a J/ψ, we extract the first
measurement of the total single b-hadron cross section down
to zero transverse momentum at √s = 1960 GeV. We find the
total single b-hadron cross section integrated over all
transverse momenta for b hadrons in the rapidity range |y|
< 0.6 to be 17.6 ± 0.4(stat) -2.3+2.5(syst) μb. © 2005
The American Physical Society.},
Doi = {10.1103/PhysRevD.71.032001},
Key = {fds340915}
}
@article{fds308524,
Author = {Aaltonen, T and others},
Title = {Measurement of the k[sub T] Distribution of Particles in
Jets Produced in p[overline p] Collisions at sqrt(s) = 1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {23},
Pages = {232002},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.232002},
Abstract = {We present a measurement of the transverse momentum with
respect to the jet axis (k(t)) of particles in jets produced
in pp collisions at sqrt(s)=1.96 TeV. Results are obtained
for charged particles in a cone of 0.5 radians around the
jet axis in events with dijet invariant masses between 66
and 737 GeV/c(2). The experimental data are compared to
theoretical predictions obtained for fragmentation partons
within the framework of resummed perturbative QCD using the
modified leading log and next-to-modified leading log
approximations. The comparison shows that trends in data are
successfully described by the theoretical predictions,
indicating that the perturbative QCD stage of jet
fragmentation is dominant in shaping basic jet
characteristics.},
Doi = {10.1103/physrevlett.102.232002},
Key = {fds308524}
}
@article{fds308830,
Author = {al, FAE},
Title = {Measurement of the Lepton Charge Asymmetry in W-Boson Decays
Produced in pp Collisions},
Journal = {Physical Review Letters},
Volume = {81},
Number = {26},
Pages = {5754},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.5754},
Abstract = {We describe a measurement of the charge asymmetry of leptons
from W-boson decays in the rapidity range 0 < |yl| < 2.5
using W → eν,μν events from 110±7pb-1 of data
collected by the CDF detector during 1992–1995. The
asymmetry data constrain the ratio of d and u quark momentum
distributions in the proton over the x range of 0.006 to
0.34 at Q2 ≈ M2W. The asymmetry predictions that use
parton distribution functions obtained from previously
published CDF data in the central rapidity region (0.0 <
|yl| < 1.1) do not agree with the new data in the large
rapidity region (|yl| > 1.1). © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.81.5754},
Key = {fds308830}
}
@article{fds308304,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Measurement of the leptonic asymmetry in tt̄ events
produced in pp̄ collisions at √s=1.96
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.88.072003},
Abstract = {We measure the asymmetry in the charge-weighted rapidity
qyℓ of the lepton in semileptonic tt̄ decays recorded
with the CDF II detector using the full Tevatron Run II
sample, corresponding to an integrated luminosity of 9.4
fb-1. A parametrization of the asymmetry as a function of
qyℓ is used to correct for the finite acceptance of the
detector and recover the production-level asymmetry. The
result of AFBℓ=0.094-0.029+0.032 is to be compared to the
standard model next-to-leading-order prediction of
AFBℓ=0.038±0.003. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.072003},
Key = {fds308304}
}
@article{fds308702,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann,
JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko,
I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and da Costa, JG and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko,
S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko,
I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann,
SE and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu,
R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller,
L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
C and Pompos, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
D},
Title = {Measurement of the lifetime difference between Bs mass
eigenstates.},
Journal = {Physical review letters},
Volume = {94},
Number = {10},
Pages = {101803},
Year = {2005},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.94.101803},
Abstract = {We present measurements of the lifetimes and polarization
amplitudes for B(0)(s)-->J/psiphi and B(0)(d)-->J/psiK(*0)
decays. Lifetimes of the heavy and light mass eigenstates in
the B(0)(s) system are separately measured for the first
time by determining the relative contributions of amplitudes
with definite CP as a function of the decay time. Using
203+/-15 B(0)(s) decays we obtain tau(L) =
(1.05(+0.16)(-0.13) +/- 0.02) ps and tau(H) =
(2.07(+0.58)(-0.46) +/- 0.03) ps. Expressed in terms of the
difference DeltaGamma(s) and average Gamma(s), of the decay
rates of the two eigenstates, the results are
DeltaGamma(s)/Gamma(s) = (65(+25)(-33) +/- 1)% and
DeltaGamma(s) = (0.47(+0.19)(-0.24) +/- 0.01)
ps(-1).},
Doi = {10.1103/physrevlett.94.101803},
Key = {fds308702}
}
@article{fds308881,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
S and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cronin-Hennessy, D and Culbertson,
R and Cunningham, JD and Daniels, T and Jongh, FD and Delchamps, S and dell'Agnello, S and dell'Orso, M and Demina, R and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Dunn, A and Eddy, N and Einsweiler,
K and Elias, JE and Ely, R and Jr, EE and Errede, D and Errede, S and Fan, Q and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi,
M and Freeman, J and Friedman, J and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold,
M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Guo,
RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Hardman, AD and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Hayashi, E and Heinrich, J and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes, R and Huston, J and Huth, J and Hylen, J and Ikeda, H and Incagli,
M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and Jensen, H and Joshi, U and Kadel, RW and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Keeble, L and Kelley, K and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kharadia,
B and Kim, BJ and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Korytov, A and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuwabara, T and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and Compte, TL and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lu, J and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi,
E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Mitsushio, H and Miyamoto,
T and Miyashita, S and Moggi, N and Morita, Y and Mueller, J and Mukherjee,
A and Muller, T and Murat, P and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ninomiya, M and Nodulman, L and Oh, SH and Ohl, KE and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Oliveira, R and Olsen, J and Pagliarone, C and Paoletti,
R and Papadimitriou, V and Pappas, SP and Park, S and Parri, A and Patrick,
J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters,
MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Romano, J and Rosenson, L and Roser, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Scarpine, V and Schlabach, P and Schmidt, EE and Schmidt, MP and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Sganos, G and Shapiro, MD and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Snider, FD and Song, T and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Strahl, K and Strait, J and Ströhmer, R and Stuart, D and Sullivan, G and Soumarokov, A and Sumorok, K and Suzuki, J and Takada, T and Takahashi, T and Takano, T and Takikawa, K and Tamura, N and Tartarelli, F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Uemura, N and Ukegawa, F and Unal, G and Brink, SCVD and III, SV and Velev, G and Vidal,
R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wahl,
J and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel,
H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Wolinski, D and Wolinski,
J and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh,
GP and Yeh, P and Yin, M and Yoh, J and Yosef, C and Yoshida, T and Yovanovitch, D and Yu, I and Yu, L and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, W and Zucchelli, S},
Title = {Measurement of the lifetime of the Bs0
meson using the exclusive decay mode Bs0
→ J/ψ φ},
Journal = {Physical Review Letters},
Volume = {77},
Number = {10},
Pages = {1945-1949},
Year = {1996},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.77.1945},
Abstract = {The lifetime of the Bs0 meson is measured using the
exclusive decay mode Bs0 → J / ψ φ, where J/ψ →
μ+μ- and φ → K+K-. The data sample consists of 110 pb-1
of p p̄ collisions at √s = 1.8 TeV, collected by the CDF
detector at the Fermilab Tevatron collider during 1992-1995.
We find 58 ± 12 signal events, and the Bs0 meson lifetime
is determined to be τBs0; = 1.34-0.19+0.23(stat) ±
0.05(syst) ps. This result is consistent with previous
measurements of the Bs0, B+, and Bd0 meson lifetimes and
with theoretical predictions.},
Doi = {10.1103/PhysRevLett.77.1945},
Key = {fds308881}
}
@article{fds321350,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Measurement of the low-mass Drell-Yan differential cross
section at √s = 7 TeV using the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {6},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP06(2014)112},
Abstract = {The differential cross section for the process Z/γ * →
ℓℓ (ℓ = e, μ) as a function of dilepton invariant
mass is measured in pp collisions at √s = 7 TeV at the LHC
using the ATLAS detector. The measurement is performed in
the e and μ channels for invariant masses between 26 GeV
and 66 GeV using an integrated luminosity of 1.6 fb -1
collected in 2011 and these measurements are combined. The
analysis is extended to invariant masses as low as 12 GeV in
the muon channel using 35 pb-1 of data collected in 2010.
The cross sections are determined within fiducial acceptance
regions and corrections to extrapolate the measurements to
the full kinematic range are provided. Next-to-next-to-leading-
order QCD predictions provide a significantly better
description of the results than next-to-leading-order QCD
calculations, unless the latter are matched to a parton
shower calculation. [Figure not available: see fulltext.] ©
2014 The Author(s).},
Doi = {10.1007/JHEP06(2014)112},
Key = {fds321350}
}
@article{fds308440,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of the Mass Difference between $t$ and
$\overline{t}$ Quarks},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {15},
Pages = {152001},
Publisher = {American Physical Society},
Year = {2011},
Month = {April},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.152001},
Abstract = {We present a direct measurement of the mass difference
between t and t quarks using tt candidate events in the
lepton+jets channel, collected with the CDF II detector at
Fermilab's 1.96 TeV Tevatron pp Collider. We make an event
by event estimate of the mass difference to construct
templates for top quark pair signal events and background
events. The resulting mass difference distribution of data
is compared to templates of signals and background using a
maximum likelihood fit. From a sample corresponding to an
integrated luminosity of 5.6 fb(-1), we measure a mass
difference, ΔM(top) = M(t) - M(t) = -3.3 ± 1.4(stat) ±
1.0(syst) GeV/c2, approximately 2 standard deviations
away from the CPT hypothesis of zero mass
difference.},
Doi = {10.1103/PhysRevLett.106.152001},
Key = {fds308440}
}
@article{fds308289,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
JF},
Title = {Measurement of the mass difference between top and anti-top
quarks in pp collisions at √s=7 TeV using the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {728},
Pages = {363-379},
Publisher = {Elsevier BV},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2013.12.010},
Abstract = {A measurement of the mass difference between top and
anti-top quarks is presented. In a 4.7 fb−1 data sample of
proton–proton collisions at s=7 TeV recorded with the
ATLAS detector at the LHC, events consistent with tt¯
production and decay into a single charged lepton final
state are reconstructed. For each event, the mass difference
between the top and anti-top quark candidate is calculated.
A two b-tag requirement is used in order to reduce the
background contribution. A maximum likelihood fit to these
per-event mass differences yields Δm≡mt−mt¯=0.67±0.61(stat)±0.41(syst)
GeV, consistent with CPT invariance.},
Doi = {10.1016/j.physletb.2013.12.010},
Key = {fds308289}
}
@article{fds308378,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and Barbaro,
PD and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Canto,
AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Ramos, JPF and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Garfinkel, AF and Garosi,
P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and López, OG and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare,
M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov,
A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Fernández, IR and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov,
A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, WM and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S},
Title = {Measurement of the mass difference between top and antitop
quarks},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {5},
Pages = {052013},
Year = {2013},
url = {http://dx.doi.org/10.1103/PhysRevD.87.052013},
Abstract = {We present a measurement of the mass difference between top
(t) and antitop (t̄) quarks using tt̄ candidate events
reconstructed in the final state with one lepton and
multiple jets. We use the full data set of Tevatron
√s=1.96 TeV proton-antiproton collisions recorded by the
CDF II detector, corresponding to an integrated luminosity
of 8.7 fb-1. We estimate event by event the mass difference
to construct templates for top pair signal events and
background events. The resulting mass difference
distribution in data compared to signal and background
templates using a likelihood fit yields ΔMtop=Mt-Mt̄=-1.95±1.11(stat)
±0.59(syst) GeV/c2 and is in agreement with the standard
model prediction of no mass difference. © 2013 American
Physical Society.},
Doi = {10.1103/PhysRevD.87.052013},
Key = {fds308378}
}
@article{fds331630,
Author = {Collaboration, DAEACDF},
Title = {Measurement of the mass difference m(D+s)-m(D+) at CDF
II},
Journal = {Physical Review},
Volume = {D68},
Number = {7},
Pages = {072004},
Publisher = {American Physical Society (APS)},
Year = {2003},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.68.072004},
Abstract = {We present a measurement of the mass difference
m(D+s)-m(D+), where both the D+s and D+ are reconstructed in
the phi pi + decay channel. This measurement uses 11.6 pb-1
of data collected by CDF II using the new displaced-track
trigger. The mass difference is found to bem(D+s)-
m(D+)=99.41±0.38(stat)±0.21(syst) MeV/c2.},
Doi = {10.1103/PhysRevD.68.072004},
Key = {fds331630}
}
@article{fds308884,
Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cen, Y and Cervelli, F and Chao, HY and Chapman, J and Cheng, M-T and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cunningham, JD and Daniels, T and DeJongh, F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dickson, M and Dittmann,
JR and Donati, S and Drucker, RB and Dunn, A and Einsweiler, K and Elias,
JE and Ely, R and Engels, E and Eno, S and Errede, D and Errede, S and Fan, Q and Farhat, B and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman, J and Frisch, H and Fry, A and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro, M and Garfinkel, AF and Geer, S and Gerdes, DW and Giannetti,
P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold, M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Grewal, A and Groer, L and Grosso-Pilcher, C and Haber,
C and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Heinrich, J and Cronin-Hennessy, D and Hollebeek, R and Holloway, L and Holscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes,
R and Hurst, P and Huston, J and Huth, J and Hylen, J and Incagli, M and Incandela, J and Iso, H and Jensen, H and Jessop, CP and Joshi, U and Kadel, RW and Kajfasz, E and Kamon, T and Kaneko, T and Kardelis, DA and Kasha, H and Kato, Y and Keeble, L and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Loomis, C and Long, O and Loreti, M and Low, EH and Lu, J and Lucchesi, D and Luchini,
CB and Lukens, P and Lys, J and Maas, P and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Michail, G and Mikamo, S and Miller, M and Miller, R and Mimashi, T and Miscetti, S and Mishina, M and Mitsushio, H and Miyashita, S and Morita, Y and Moulding,
S and Mueller, J and Mukherjee, A and Muller, T and Musgrave, P and Nakae,
LF and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Nodulman, L and Ogawa, S and Oh, SH and Ohl, KE and Oishi, R and Okusawa,
T and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Park, S and Patrick, J and Pauletta, G and Paulini, M and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Plunkett, R and Pondrom, L and Produit, N and Proudfoot, J and Ptohos,
F and Punzi, G and Ragan, K and Rimondi, F and Ristori, L and Roach-Bellino, M and Robertson, WJ and Rodrigo, T and Romano, J and Rosenson, L and Sakumoto, WK and Saltzberg, D and Sansoni, A and Scarpine, V and Schindler, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schneider, O and Sciacca, GF and Scribano, A and Segler,
S and Seidel, S and Seiya, Y and Sganos, G and Sgolacchia, A and Shapiro,
M and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Smith, DA and Snider, FD and Song, L and Song, T and Spalding,
J and Spiegel, L and Sphicas, P and Stanco, L and Steele, J and Stefanini,
A and Strahl, K and Strait, J and Stuart, D and Sullivan, G and Sumorok, K and Swartz, RL and Takahashi, T and Takikawa, K and Tartarelli, F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, J and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov,
A and Tkaczyk, S and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Tseng, J and Turcotte, M and Turini, N and Uemura, N and Ukegawa, F and Unal, G and Brink, SCVD and Vejcik, S and Vidal, R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wainer, N and Walker, RC and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, G and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and Wester, WC and Westhusing, T and Wicklund,
AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Wolinski, J and Wu, DY and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef, C and Yoshida, T and Yovanovitch, D and Yu, I and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, S and Zhang, W and Zucchelli, S},
Title = {Measurement of the mass of the Bs0
meson},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {53},
Number = {7},
Pages = {3496-3505},
Year = {1996},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/physrevd.53.3496},
Abstract = {We measure the mass of the B0s meson by reconstructing the
decay chain B0s→J/ψφ, J/ψ→µ+µ-, and φ→K+K-. The
data are obtained from 19.3 pb-1 of integrated luminosity of
pp collisions at √s=1.8 TeV using the Collider Detector at
Fermilab. A sample of 80 000 inclusive J/ψ→µ+µ- events
is used to study systematic biases in track reconstruction
and to calibrate the momentum scale. We reconstruct the
kinematically similar decays B+→J/ψK+ and B0→J/ψK*0 to
study the mass measurement technique used for the B0s meson.
Based on the observation of 32 ± 6 candidates, the mass of
the B0s meson is measured to be 5369.9 ± 2.3 ± 1.3 MeV/c2
and the mass difference between B0s and the average mass of
B+ and B0 is determined to be 89.7 ± 2.7 ± 1.2 MeV/c2. ©
1996 The American Physical Society.},
Doi = {10.1103/physrevd.53.3496},
Key = {fds308884}
}
@article{fds308399,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli,
M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F and D'errico, M and Di Canto,
A},
Title = {Measurement of the masses and widths of the bottom baryons
Σb± and Σb*±},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.85.092011},
Abstract = {Using data from pp̄ collisions at √s=1.96TeV recorded by
the CDF II detector at the Fermilab Tevatron, we present
improved measurements of the masses and first measurements
of natural widths of the four bottom baryon resonance states
Σb+, Σb*+ and Σb-, Σb*-. These states are fully
reconstructed in their decay modes to Λb0π ± where
Λb0→Λc+π - with Λc+→pK -π +. The analysis is based
on a data sample corresponding to an integrated luminosity
of 6.0fb -1 collected by an online event selection based on
tracks displaced from the pp̄ interaction point. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.85.092011},
Key = {fds308399}
}
@article{fds314196,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer,
S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao,
T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel,
R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa,
T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman,
MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert,
B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert,
K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu,
V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri,
F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF},
Title = {Measurement of the moments of the hadronic invariant mass
distribution in semileptonic B decays},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {5},
Pages = {1-9},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.051103},
Abstract = {Using 180 pb -1 of data collected with the CDF II detector
at the Tevatron, we measure the first two moments of the
hadronic invariant mass-squared distribution in charmed
semileptonic B decays. From these we determine the
nonperturbative Heavy Quark Effective Theory parameters Λ
and λ 1 used to relate the B meson semileptonic branching
ratio to the CKM matrix element |V cb|. For a minimum lepton
momentum of 0.7 GeV/c in the B rest frame we measure the
first two moments of the D** → D (*)π component to be
〈m D**2〉 = (5.83 ± 0.16 stat ± 0.08 syst) GeV 2/c 4
and 〈(m D**2 - 〈m D**2〉) 2〉 = (1.30 ± 0.69 stat ±
0.22 syst) GeV 4/c 8. Combining these with the discrete mass
terms from the D and D* mesons, we find the total moments to
be 〈M Ξc2〉 - m̄ D2 = (0.467 ± 0.038 stat ± 0.068
syst GeV 2/c 4 and 〈(M Ξc2 - 〈M Ξc2〉) 2〉 = (1.05
± 0.26 stat ± 0.13 syst) GeV 4/c 8, where m̄ D is the
spin-averaged D mass. The systematic error is dominated by
the uncertainties in the world-average branching ratios used
to combine the D, D*, and D** contributions. The analysis
makes no assumptions about the shape or resonant structure
of the D** → D (*)π invariant mass distribution. © 2005
The American Physical Society.},
Doi = {10.1103/PhysRevD.71.051103},
Key = {fds314196}
}
@article{fds321364,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, M and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Measurement of the muon reconstruction performance of the
ATLAS detector using 2011 and 2012 LHC proton-proton
collision data.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {11},
Pages = {3130},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3130-x},
Abstract = {This paper presents the performance of the ATLAS muon
reconstruction during the LHC run with [Formula: see text]
collisions at [Formula: see text]-8 TeV in 2011-2012,
focusing mainly on data collected in 2012. Measurements of
the reconstruction efficiency and of the momentum scale and
resolution, based on large reference samples of [Formula:
see text], [Formula: see text] and [Formula: see text]
decays, are presented and compared to Monte Carlo
simulations. Corrections to the simulation, to be used in
physics analysis, are provided. Over most of the covered
phase space (muon [Formula: see text] and [Formula: see
text] GeV) the efficiency is above [Formula: see text] and
is measured with per-mille precision. The momentum
resolution ranges from [Formula: see text] at central
rapidity and for transverse momentum [Formula: see
text] GeV, to [Formula: see text] at large rapidity and
[Formula: see text] GeV. The momentum scale is known with
an uncertainty of [Formula: see text] to [Formula: see text]
depending on rapidity. A method for the recovery of final
state radiation from the muons is also presented.},
Doi = {10.1140/epjc/s10052-014-3130-x},
Key = {fds321364}
}
@article{fds375949,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Measurement of the nuclear modification factor of b-jets in
5.02 TeV Pb+Pb collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11427-9},
Abstract = {This paper presents a measurement of b-jet production in
Pb+Pb and pp collisions at sNN=5.02 TeV with the ATLAS
detector at the LHC. The measurement uses 260 pb - 1 of pp
collisions collected in 2017 and 1.4 nb - 1 of Pb+Pb
collisions collected in 2018. In both collision systems,
jets are reconstructed via the anti- kt algorithm. The
b-jets are identified from a sample of jets containing muons
from the semileptonic decay of b-quarks using template fits
of the muon momentum relative to the jet axis. In pp
collisions, b-jets are reconstructed for radius parameters
R= 0.2 and R= 0.4 , and only R= 0.2 jets are used in Pb+Pb
collisions. For comparison, inclusive R= 0.2 jets are also
measured using 1.7 nb - 1 of Pb+Pb collisions collected in
2018 and the same pp collision data as the b-jet
measurement. The nuclear modification factor, RAA , is
calculated for both b-jets and inclusive jets with R= 0.2
over the transverse momentum range of 80–290 GeV. The
nuclear modification factor for b-jets decreases from
peripheral to central collisions. The ratio of the b-jet RAA
to inclusive jet RAA is also presented and suggests that the
RAA for b-jets is larger than that for inclusive jets in
central Pb+Pb collisions. The measurements are compared with
theoretical calculations and suggest a role for mass and
colour-charge effects in partonic energy loss in heavy-ion
collisions.},
Doi = {10.1140/epjc/s10052-023-11427-9},
Key = {fds375949}
}
@article{fds308273,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Measurement of the parity-violating asymmetry parameter αb
and the helicity amplitudes for the decay Λb0 →j /ψ Λ0
with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.89.092009},
Abstract = {A measurement of the parity-violating decay asymmetry
parameter, αb, and the helicity amplitudes for the decay
Λb0→J/ψ(μ+μ-)Λ0(pπ-) is reported. The analysis is
based on 1400 Λb0 and Λ¯b0 baryons selected in 4.6 fb-1
of proton-proton collision data with a center-of-mass energy
of 7 TeV recorded by the ATLAS experiment at the LHC. By
combining the Λb0 and Λ¯b0 samples under the assumption
of CP conservation, the value of αb is measured to be
0.30±0.16(stat)±0.06(syst). This measurement provides a
test of theoretical models based on perturbative QCD or
heavy-quark effective theory.},
Doi = {10.1103/PhysRevD.89.092009},
Key = {fds308273}
}
@article{fds322007,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Measurement of the photon identification efficiencies with
the ATLAS detector using LHC Run-1 data.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {12},
Pages = {666},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4507-9},
Abstract = {The algorithms used by the ATLAS Collaboration to
reconstruct and identify prompt photons are described.
Measurements of the photon identification efficiencies are
reported, using 4.9 fb[Formula: see text] of pp collision
data collected at the LHC at [Formula: see text] [Formula:
see text] and 20.3 fb[Formula: see text] at [Formula: see
text] [Formula: see text]. The efficiencies are measured
separately for converted and unconverted photons, in four
different pseudorapidity regions, for transverse momenta
between 10 [Formula: see text] and 1.5 [Formula: see
text]. The results from the combination of three data-driven
techniques are compared to the predictions from a simulation
of the detector response, after correcting the
electromagnetic shower momenta in the simulation for the
average differences observed with respect to data.
Data-to-simulation efficiency ratios used as correction
factors in physics measurements are determined to account
for the small residual efficiency differences. These factors
are measured with uncertainties between 0.5% and 10% in
7 [Formula: see text] data and between 0.5% and 5.6% in
8 [Formula: see text] data, depending on the photon
transverse momentum and pseudorapidity.},
Doi = {10.1140/epjc/s10052-016-4507-9},
Key = {fds322007}
}
@article{fds308738,
Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
JY and Chung, W and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
J and Culbertson, R and Dagenhart, D and D’Auria, S and Barbaro, P and Cecco, S and Dell’Agnello, S and Dell’Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, D and Derwent, PF and Dionisi, C and Dittmann, JR and Dominguez, A and Donati, S and D’Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede,
S},
Title = {Measurement of the polar-angle distribution of leptons from
W boson decay as a function of the W transverse momentum in
[Formula Presented] collisions at [Formula
Presented]},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {70},
Number = {3},
Pages = {032004-1-032004-21},
Publisher = {American Physical Society (APS)},
Year = {2004},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.70.032004},
Abstract = {We present a measurement of the polar-angle distribution of
leptons from W boson decay, as a function of the W
transverse momentum. The measurement uses an [Formula
Presented] sample of [Formula Presented] collisions at
[Formula Presented] collected by the CDF detector and
includes data from both the [Formula Presented] and [Formula
Presented] decay channels. We fit the W boson transverse
mass distribution to a set of templates from a Monte Carlo
event generator and detector simulation in several ranges of
the W transverse momentum. The measurement agrees with the
standard model expectation, whereby the ratio of
longitudinally to transversely polarized W bosons, in the
Collins-Soper W rest frame, increases with the W transverse
momentum at a rate of approximately 15% per [Formula
Presented]. © 2004 The American Physical
Society.},
Doi = {10.1103/PhysRevD.70.032004},
Key = {fds308738}
}
@article{fds375913,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport, PP and Aloisio,
A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez
Fernandez, A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH},
Title = {Measurement of the polarisation of W bosons produced in
top-quark decays using dilepton events at s=13 TeV with the
ATLAS experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137829},
Abstract = {A measurement of the polarisation of W bosons produced in
top-quark decays is presented, using proton–proton
collision data at a centre-of-mass energy of s=13 TeV. The
data were collected by the ATLAS detector at the Large
Hadron Collider and correspond to an integrated luminosity
of 139 fb−1. The measurement is performed selecting tt¯
events decaying into final states with two charged leptons
(electrons or muons) and at least two b-tagged jets. The
polarisation is extracted from the differential
cross-section distribution of the cosθ⁎ variable,
where θ⁎ is the angle between the momentum direction of
the charged lepton from the W boson decay and the reversed
momentum direction of the b-quark from the top-quark decay,
both calculated in the W boson rest frame. Parton-level
results, corrected for the detector acceptance and
resolution, are presented for the cosθ⁎ angle. The
measured fractions of longitudinal, left- and right-handed
polarisation states are found to be f0=0.684±0.005(stat.)±0.014(syst.),
fL=0.318±0.003(stat.)±0.008(syst.) and
fR=−0.002±0.002(stat.)±0.014(syst.), in agreement with
the Standard Model prediction.},
Doi = {10.1016/j.physletb.2023.137829},
Key = {fds375913}
}
@article{fds308900,
Author = {al, FAE},
Title = {Measurement of the polarization in the decays
b-d-]j/psi-k-(asterisk-0) and bs-]j/psi-phi},
Journal = {Phys. Rev. Lett.},
Volume = {75},
Number = {17},
Pages = {3068-3072},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevLett.75.3068},
Abstract = {This Letter reports on measurements of the longitudinal
polarization fractions in the decays Bd→J/ψ K*0 and
Bs→J/ψ φ using data collected with the Collider Detector
at Fermilab. Bd mesons are reconstructed through the decay
chain Bd→J/ψ K*0, J/ψ→μ+μ-, K*0→K+π-. A sample of
65±10 Bd events is used to obtain a longitudinal
polarization fraction of γL/γ=0.65±0.10(stat)±0.04(syst).
Bs mesons are reconstructed through the decay chain
Bs→J/ψ φ, J/ψ→μ+μ-, φ→K+K-. A sample of 19±5 Bs
events is used to obtain the result γL/γ=0.56±0.21(stat)-0.04+0.
02(syst). © 1995 The American Physical Society.},
Doi = {10.1103/PhysRevLett.75.3068},
Key = {fds308900}
}
@article{fds321246,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of the production and differential cross
sections of W+W- bosons in association
with jets in pp¯ collisions at √s = 1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.91.111101},
Abstract = {We present a measurement of the W-boson-pair production
cross section in pp¯ collisions at 1.96 TeV center-of-mass
energy and the first measurement of the differential cross
section as a function of jet multiplicity and leading-jet
energy. The W+W- cross section is measured in the final
state comprising two charged leptons and neutrinos, where
either charged lepton can be an electron or a muon. Using
data collected by the CDF experiment corresponding to
9.7fb-1 of integrated luminosity, a total of 3027 collision
events consistent with W+W- production are observed with an
estimated background contribution of 1790 ± 190 events. The
measured total cross section is σ(pp¯ → W+W-)= 14.0 ±
0.6 (stat)-1.0+1.2 (syst) ± 0.8 (lumi) pb, consistent with
the standard model prediction.},
Doi = {10.1103/PhysRevD.91.111101},
Key = {fds321246}
}
@article{fds321272,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat,
A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin,
M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell,
WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
A},
Title = {Measurement of the production and lepton charge asymmetry of
[Formula: see text] bosons in Pb+Pb collisions at [Formula:
see text] with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {1},
Pages = {23},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3231-6},
Abstract = {A measurement of [Formula: see text] boson production in
lead-lead collisions at [Formula: see text] is presented. It
is based on the analysis of data collected with the ATLAS
detector at the LHC in 2011 corresponding to an integrated
luminosity of 0.14 [Formula: see text] and 0.15 [Formula:
see text] in the muon and electron decay channels,
respectively. The differential production yields and lepton
charge asymmetry are each measured as a function of the
average number of participating nucleons [Formula: see text]
and absolute pseudorapidity of the charged lepton. The
results are compared to predictions based on
next-to-leading-order QCD calculations. These measurements
are, in principle, sensitive to possible nuclear
modifications to the parton distribution functions and also
provide information on scaling of [Formula: see text] boson
production in multi-nucleon systems.},
Doi = {10.1140/epjc/s10052-014-3231-6},
Key = {fds321272}
}
@article{fds308363,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E and Arik, M and Armbruster, AJ},
Title = {Measurement of the production cross section of jets in
association with a Z boson in pp collisions at √s=7 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {7},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP07(2013)032},
Abstract = {Measurements of the production of jets of particles in
association with a Z boson in pp collisions at √s=7 TeV
are presented, using data corresponding to an integrated
luminosity of 4.6 fb-1 collected by the ATLAS experiment at
the Large Hadron Collider. Inclusive and differential jet
cross sections in Z events, with Z decaying into electron or
muon pairs, are measured for jets with transverse momentum p
T > 30 GeV and rapidity |y| < 4.4. The results are compared
to next-to-leading-order perturbative QCD calculations, and
to predictions from different Monte Carlo generators based
on leading-order and next-to-leading-order matrix elements
supplemented by parton showers. [Figure not available: see
fulltext.] © 2013 CERN for the benefit of the ATLAS
collaboration.},
Doi = {10.1007/JHEP07(2013)032},
Key = {fds308363}
}
@article{fds365373,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala,
J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada
Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S},
Title = {Measurement of the production cross section of pairs of
isolated photons in pp collisions at 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2021)169},
Abstract = {A measurement of prompt photon-pair production in
proton-proton collisions at s = 13 TeV is presented. The
data were recorded by the ATLAS detector at the LHC with an
integrated luminosity of 139 fb−1. Events with two photons
in the well-instrumented region of the detector are
selected. The photons are required to be isolated and have a
transverse momentum of pT,γ1(2)> 40 (30) GeV for the
leading (sub-leading) photon. The differential cross
sections as functions of several observables for the
diphoton system are measured and compared with theoretical
predictions from state-of-the-art Monte Carlo and
fixed-order calculations. The QCD predictions from
next-to-next-to-leading-order calculations and multi-leg
merged calculations are able to describe the measured
integrated and differential cross sections within
uncertainties, whereas lower-order calculations show
significant deviations, demonstrating that higher-order
perturbative QCD corrections are crucial for this process.
The resummed predictions with parton showers additionally
provide an excellent description of the low
transverse-momentum regime of the diphoton system. [Figure
not available: see fulltext.].},
Doi = {10.1007/JHEP11(2021)169},
Key = {fds365373}
}
@article{fds308279,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
M},
Title = {Measurement of the production cross section of prompt J/ψ
mesons in association with a W± boson in pp collisions at
√s = 7 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {4},
Publisher = {Springer Nature},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2014)172},
Abstract = {The process pp → W±J/ψ provides a powerful probe of the
production mechanism of charmonium in hadronic collisions,
and is also sensitive to multiple parton interactions in the
colliding protons. Using the 2011 ATLAS dataset of 4.5 fb-1
of p s = 7TeV pp collisions at the LHC, the first
observation is made of the production of W± + prompt J/
events in hadronic collisions, using W± → μ and J/ψ →
μ+μ-. A yield of 27.4±7.5 -6.5 W± + prompt J/ψ events
is observed, with a statistical significance of 5.1. The
production rate as a ratio to the inclusive W± boson
production rate is measured, and the double parton
scattering contribution to the cross section is estimated.
Copyright CERN, for the benefit of the ATLAS
Collaboration.},
Doi = {10.1007/JHEP04(2014)172},
Key = {fds308279}
}
@article{fds321210,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of the production cross-section of a single top
quark in association with a W boson at 8 TeV with the ATLAS
experiment},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {1},
Pages = {1-48},
Publisher = {Springer Nature},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2016)064},
Abstract = {The cross-section for the production of a single top quark
in association with a W boson in proton-proton collisions at
√s = 8TeV is measured. The dataset corresponds to an
integrated luminosity of 20.3 fb−1, collected by the ATLAS
detector in 2012 at the Large Hadron Collider at CERN.
Events containing two leptons and one central b-jet are
selected. The W t signal is separated from the backgrounds
using boosted decision trees, each of which combines a
number of discriminating variables into one classifier.
Production of W t events is observed with a significance of
7.7σ. The cross-section is extracted in a profile
likelihood fit to the classifier output distributions. The W
t cross-section, inclusive of decay modes, is measured to be
23.0 ± 1.3(stat.)− 3.5+ 3.2(syst.)±1.1(lumi.) pb. The
measured cross-section is used to extract a value for the
CKM matrix element |Vtb| of 1.01 ± 0.10 and a lower limit
of 0.80 at the 95% confidence level. The cross-section for
the production of a top quark and a W boson is also measured
in a fiducial acceptance requiring two leptons with pT> 25
GeV and |η| < 2.5, one jet with pT> 20 GeV and |η| < 2.5,
and ETmiss > 20 GeV, including both W t and top-quark pair
events as signal. The measured value of the fiducial
cross-section is 0.85 ± 0.01(stat.)− 0.07+
0.07(syst.)±0.03(lumi.) pb.},
Doi = {10.1007/JHEP01(2016)064},
Key = {fds321210}
}
@article{fds376250,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Bourdarios, CA and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Measurement of the production cross-section of J/ψ and
ψ(2S) mesons in pp collisions at s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {84},
Number = {2},
Year = {2024},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-024-12439-9},
Abstract = {Measurements of the differential production cross-sections
of prompt and non-prompt J/ψ and ψ(2S) mesons with
transverse momenta between 8 and 360 GeV and rapidity in
the range |y|<2 are reported. Furthermore, measurements of
the non-prompt fractions of J/ψ and ψ(2S), and the prompt
and non-prompt ψ(2S)-to-J/ψ production ratios, are
presented. The analysis is performed using 140 fb-1 of
s=13 TeV pp collision data recorded by the ATLAS detector
at the LHC during the years 2015–2018.},
Doi = {10.1140/epjc/s10052-024-12439-9},
Key = {fds376250}
}
@article{fds321351,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
M},
Title = {Measurement of the production of a W boson in association
with a charm quark in pp collisions at √s = 7TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {5},
Pages = {1-67},
Publisher = {Springer Nature},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2014)068},
Abstract = {The production of a W boson in association with a single
charm quark is studied using 4.6 fb-1 of pp collision data
at √s = 7TeV collected with the ATLAS detector at the
Large Hadron Collider. In events in which a W boson decays
to an electron or muon, the charm quark is tagged either by
its semileptonic decay to a muon or by the presence of a
charmed meson. The integrated and differential cross
sections as a function of the pseudorapidity of the lepton
from the W-boson decay are measured. Results are compared to
the predictions of next-to-leading-order QCD calculations
obtained from various parton distribution function
parameterisations. The ratio of the strange-to-down
sea-quark distributions is determined to be 0.96+-00.30 at
Q2 = 1.9 GeV, which supports the hypothesis of an
SU(3)-symmetric composition of the light-quark sea.
Additionally the cross-section ratio σ(W+ + c)/σ(W- +c) is
compared to the predictions obtained using parton
distribution function parameterisations with different
assumptions about the s–s quark asymmetry.},
Doi = {10.1007/JHEP05(2014)068},
Key = {fds321351}
}
@article{fds375924,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori, G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang, R and Zhang, J and Berlendis,
S and Cheu, E and Cui, Z and Ghosh, A and Johns, KA and Lampl, W and Lindley,
RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou,
H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai,
G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost, M and Unal, M and Huseynov, N},
Title = {Measurement of the production of a W boson in association
with a charmed hadron in pp collisions at √s=13 TeV with
the ATLAS detector},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032012},
Abstract = {The production of a W boson in association with a single
charm quark is studied using 140 fb - 1 of s = 13 TeV
proton-proton collision data collected with the ATLAS
detector at the Large Hadron Collider. The charm quark is
tagged by the presence of a charmed hadron reconstructed
with a secondary-vertex fit. The W boson is reconstructed
from the decay to either an electron or a muon and the
missing transverse momentum present in the event. The
charmed mesons reconstructed are D + → K - π + π + and D
* + → D 0 π + → ( K - π + ) π + and the charge
conjugate decays in the fiducial regions where p T ( e , μ
) > 30 GeV , | η ( e , μ ) | < 2.5 , p T ( D ( * ) ) > 8
GeV , and | η ( D ( * ) ) | < 2.2 . The integrated and
normalized differential cross sections as a function of the
pseudorapidity of the lepton from the W boson decay, and of
the transverse momentum of the charmed hadron, are extracted
from the data using a profile likelihood fit. The measured
total fiducial cross sections are σ fid OS - SS ( W - + D +
) = 50.2 ± 0.2 ( stat ) - 2.3 + 2.4 ( syst ) pb , σ fid OS
- SS ( W + + D - ) = 48.5 ± 0.2 ( stat ) - 2.2 + 2.3 ( syst
) pb , σ fid OS - SS ( W - + D * + ) = 51.1 ± 0.4 ( stat )
- 1.8 + 1.9 ( syst ) pb , and σ fid OS - SS ( W + + D * - )
= 50.0 ± 0.4 ( stat ) - 1.8 + 1.9 ( syst ) pb . Results are
compared with the predictions of next-to-leading-order
quantum chromodynamics calculations performed using
state-of-the-art parton distribution functions.
Additionally, the ratio of charm to anticharm production
cross sections is studied to probe the s - s ¯ quark
asymmetry. The ratio is found to be R c ± = 0.971 ± 0.006
( stat ) ± 0.011 ( syst ) . The ratio and cross-section
measurements are consistent with the predictions obtained
with parton distribution function sets that have a symmetric
s - s ¯ sea, indicating that any s - s ¯ asymmetry in the
Bjorken- x region relevant for this measurement is
small.},
Doi = {10.1103/PhysRevD.108.032012},
Key = {fds375924}
}
@article{fds331635,
Author = {al, DAE},
Title = {Measurement of the ratio of b quark production cross
sections in pp collisions at $\sqrt{s}=630$ GeV and
$\sqrt{s} = 1800 GeV},
Journal = {Physical Review},
Volume = {66},
Number = {D66},
Pages = {032002},
Publisher = {American Physical Society (APS)},
Year = {2002},
url = {http://dx.doi.org/10.1103/PhysRevD.66.032002},
Abstract = {We report a measurement of the ratio of the bottom quark
production cross section in antiproton-proton collisions at
[Formula Presented] to 1800 GeV using bottom quarks with
transverse momenta greater than 10.75 GeV identified through
their semileptonic decays and long lifetimes. The measured
ratio [Formula Presented] is in good agreement with
next-to-leading order quantum chromodynamics. © 2002 The
American Physical Society.},
Doi = {10.1103/PhysRevD.66.032002},
Key = {fds331635}
}
@article{fds308572,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
MA},
Title = {Measurement of the ratio of branching fractions B(B±→J/
ψπ±)/B(B±→J/ψK±)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.79.112003},
Abstract = {We report a measurement of the ratio of branching fractions
of the decays B±→J/ψπ± and B±→J/ψK± using the CDF
II detector at the Fermilab Tevatron Collider. The signal
from the Cabbibo-suppressed B±→J/ψπ± decay is
separated from B±→J/ψK± using the B±→J/ψK±
invariant mass distribution and the kinematical differences
of the hadron track in the two decay modes. From a sample of
220pb-1 of pp̄ collisions at s=1.96TeV, we observe 91±15
B±→J/ψπ± events together with 1883±34 B±→J/ψK±
events. The ratio of branching fractions is found to be
B(B±→J/ψπ±)/ B(B±→J/ψK±)=(4.86±0.82(stat)±0.15(syst))%.
© 2009 The American Physical Society.},
Doi = {10.1103/PhysRevD.79.112003},
Key = {fds308572}
}
@article{fds308690,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo,
T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
I and Gallinaro, M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris,
N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare,
M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser,
J and Hays, C and Heijboer, A and Heinemann, B and Heinrich, J and Herndon,
M and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato,
Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian,
C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh,
YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin,
J},
Title = {Measurement of the ratio of branching fractions
B(D0→K+π-)/ B(D0→K-π+) using the CDF II
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {74},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.74.031109},
Abstract = {We present a measurement of RB, the ratio of the branching
fraction for the rare decay D0→K+π- to that for the
Cabibbo-favored decay D0→K-π+. Charge-conjugate decays
are implicitly included. A signal of 2005±104 events for
the decay D0→K+π- is obtained using the CDF II detector
at the Fermilab Tevatron collider. The data set corresponds
to an integrated luminosity of 0.35fb-1 produced in p̄p
collisions at s=1.96TeV. Assuming no mixing, we find
RB=[4.05±0.21(stat)±0.11(syst)] ×10-3. This measurement
is consistent with the world average, and comparable in
accuracy with the best measurements from other experiments.
© 2006 The American Physical Society.},
Doi = {10.1103/PhysRevD.74.031109},
Key = {fds308690}
}
@article{fds308901,
Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cen, Y},
Title = {Measurement of the ratio sigma B(pp-bar-->W-->e nu )/ sigma
B(pp-bar-->Z0-->ee) in pp-bar collisions at sqrt s =1800
GeV.},
Journal = {Physical review. D, Particles and fields},
Volume = {52},
Number = {5},
Pages = {2624-2655},
Year = {1995},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevd.52.2624},
Abstract = {© 1995 The American Physical Society We present an analysis
of data from p p collisions at a center-of-mass energy of s
=1800 GeV. A measurement is made of the ratio RB(p pWe)/B(p
pZ0ee). The data represent 19.6 pg-1 collected by the
Collider Detector at Fermilab during the 19921993 collider
run of the Fermilab Tevatron. We find R=10.900.32(stat)0.29(syst),
and from this value we extract a measurement of the We
branching ratio (We)/(W)=0.10940.0033(stat)0.0031(syst).
From this branching ratio we set a limit on the top quark
mass of mt>62 GeV/c2 at the 95% confidence level. In
contrast with direct searches for the top quark, this limit
makes no assumptions about the allowed decay modes of the
top quark. In addition, we use a calculation of the leptonic
width (We) to obtain a value for the W total decay width:
(W)=2.0640.060(stat)0.059(syst) GeV.},
Doi = {10.1103/physrevd.52.2624},
Key = {fds308901}
}
@article{fds308913,
Author = {Abe, F and Albrow, M and Amidei, D and Anway-Wiese, C and Apollinari, G and Areti, H and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and al, E},
Title = {Measurement of the ratio σB(W→eν)σB(Z0→e+e-) in p̄p
collisions at s=1.8 TeV},
Journal = {Physical Review Letters},
Volume = {73},
Number = {2},
Pages = {220-224},
Year = {1994},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.73.220},
Abstract = {We present a measurement of the ratio σB(W→eν)σB(Z0→e+e-)
in p̄p collisions at s=1.8 TeV The data represent an
integrated luminosity of 21.7 pb-1 from the 1992-1993 run of
the Collider Detector at Fermilab. We find
σB(W→eν)σB(Z0→e+e-)=10.90±0.32(stat)±0. 29(syst).
From this value, we extract a value for the W width,
Γ(W)=2.064±0.061(stat)±0.059(syst) GeV, and the branching
ratio, Γ(W→eν)Γ(W)=0.1094±0.0033(stat)±0.0031(syst),
and we set a decay-mode-independent limit on the top quark
mass mtop>62 GeV/c2 at the 95% C.L. © 1994 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.73.220},
Key = {fds308913}
}
@article{fds308652,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Casarsa, M and Castro,
A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Cyr, D and Daronco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart,
D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher,
R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster,
GW and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay,
C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson,
A and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths,
M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic, V and Renton,
P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin, J and Slaughter,
AJ},
Title = {Measurement of the ratios of branching fractions B(Bs0→Ds-
π+π+π-)/B(B0→D-π+π+π-) and B(Bs0→Ds-π+)/
B(B0→D-π+)},
Journal = {Physical Review Letters},
Volume = {98},
Number = {6},
Pages = {061802},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevLett.98.061802},
Abstract = {Using 355pb-1 of data collected by the CDF II detector in
pp̄ collisions at s=1.96TeV at the Fermilab Tevatron, we
study the fully reconstructed hadronic decays
B(s)0→D(s)-π+ and B(s)0→D(s)- π+π+π-. We present the
first measurement of the ratio of branching fractions
B(Bs0→Ds-π+π+π-)/B(B0→D-π+π+π-)=1.
05±0.10(stat)±0.22(syst). We also update our measurement
of B(Bs0→Ds-π+)/B(B0→D-π+) to 1.13±0.08(stat)±0.
23(syst), improving the statistical uncertainty by more than
a factor of 2. We find B(Bs0→Ds-π+)=[3.8±0.3(stat)±1.3(syst)]×10-3
and B(Bs0→Ds-π+π+π-)=[8.4±0.8(stat)±3.2(syst)]
×10-3. © 2007 The American Physical Society.},
Doi = {10.1103/PhysRevLett.98.061802},
Key = {fds308652}
}
@article{fds361225,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, J and DiTuro, P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Sciverez, MG and Garfinkel, AF and Gay,
C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Costa, JGD and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper,
S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer, A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel, M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute,
M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman,
R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov,
AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori,
L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli,
S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez,
C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro,
A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro,
MD},
Title = {Measurement of the ratios of branching fractions
B(Bs0→Ds-π+)/ B(B0→D-π+) and B(B+→D̄0π+)/B(B0→D-π+)},
Journal = {Physical Review Letters},
Volume = {96},
Number = {19},
Pages = {191801},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevLett.96.191801},
Abstract = {We report an observation of the decay Bs0→Ds-π+ in pp̄
collisions at s=1.96TeV using 115pb-1 of data collected by
the CDF II detector at the Fermilab Tevatron. We observe
83±11(stat) Bs0→Ds-π+ candidates, representing a large
increase in statistics over previous measurements and the
first observation of this decay at a pp̄ collider. We
present the first measurement of the relative branching
fraction B(Bs0→Ds-π+)/B(B0→D-π+)=1.32±0.18(stat)±0.38(syst)
. We also measure B(B+→D̄0π+)/B(B0→D-π+)=1.97±0.
10(stat)±0.21(syst), which is consistent with previous
measurements. © 2006 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.96.191801},
Key = {fds361225}
}
@article{fds321199,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Measurement of the relative width difference of the
B0‐ B¯ 0 system with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {6},
Publisher = {Springer Nature},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2016)081},
Abstract = {Abstract: This paper presents the measurement of the
relative width difference ΔΓd/Γd of the B0‐ B¯ 0
system using the data collected by the ATLAS experiment at
the LHC in pp collisions at s=7 TeV and s=8 TeV and
corresponding to an integrated luminosity of 25.2 fb−1.
The value of ΔΓd/Γd is obtained by comparing the
decay-time distributions of B0 → J/ψKS and B0 →
J/ψK*0(892) decays. The result is ΔΓd/Γd = (−0.1±1.1
(stat.)± 0.9 (syst.)) × 10−2. Currently, this is the
most precise single measurement of ΔΓd/Γd. It agrees with
the Standard Model prediction and the measurements by other
experiments.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP06(2016)081},
Key = {fds321199}
}
@article{fds375904,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena,
E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster,
AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio,
S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos,
G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry,
T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov,
VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans,
G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura,
P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet,
D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A},
Title = {Measurement of the Sensitivity of Two-Particle Correlations
in pp Collisions to the Presence of Hard
Scatterings.},
Journal = {Physical review letters},
Volume = {131},
Number = {16},
Pages = {162301},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.131.162301},
Abstract = {A key open question in the study of multiparticle production
in high-energy pp collisions is the relationship between the
"ridge"-i.e., the observed azimuthal correlations between
particles in the underlying event that extend over all
rapidities-and hard or semihard scattering processes. In
particular, it is not known whether jets or their soft
fragments are correlated with particles in the underlying
event. To address this question, two-particle correlations
are measured in pp collisions at sqrt[s]=13 TeV using
data collected by the ATLAS experiment at the LHC, with an
integrated luminosity of 15.8 pb^{-1}, in two different
configurations. In the first case, charged particles
associated with jets are excluded from the correlation
analysis, while in the second case, correlations are
measured between particles within jets and charged particles
from the underlying event. Second-order flow coefficients,
v_{2}, are presented as a function of event multiplicity and
transverse momentum. These measurements show that excluding
particles associated with jets does not affect the measured
correlations. Moreover, particles associated with jets do
not exhibit any significant azimuthal correlations with the
underlying event, ruling out hard processes contributing to
the ridge.},
Doi = {10.1103/physrevlett.131.162301},
Key = {fds375904}
}
@article{fds314169,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo,
N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Galloni, C and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn,
SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hirschbuehl, D and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino,
P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon,
CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat,
P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano,
I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Measurement of the single top quark production cross section
and |Vtb| in events with one charged lepton, large missing
transverse energy, and jets at CDF.},
Journal = {Physical review letters},
Volume = {113},
Number = {26},
Pages = {261804},
Year = {2014},
Month = {December},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.113.261804},
Abstract = {We report a measurement of single top quark production in
proton-antiproton collisions at a center-of-mass energy of
sqrt[s]=1.96 TeV using a data set corresponding to
7.5 fb(-1) of integrated luminosity collected by the
Collider Detector at Fermilab. We select events consistent
with the single top quark decay process t→Wb→ℓνb by
requiring the presence of an electron or muon, a large
imbalance of transverse momentum indicating the presence of
a neutrino, and two or three jets including at least one
originating from a bottom quark. An artificial neural
network is used to discriminate the signal from backgrounds.
We measure a single top quark production cross section of
3.04(-0.53)(+0.57) pb and set a lower limit on the
magnitude of the coupling between the top quark and bottom
quark |Vtb|>0.78 at the 95% credibility level.},
Doi = {10.1103/physrevlett.113.261804},
Key = {fds314169}
}
@article{fds308574,
Author = {Aaltonen, T and others},
Title = {Measurement of the Single-Top-Quark Production Cross Section
at CDF},
Journal = {Physical Review Letters},
Volume = {101},
Number = {25},
Pages = {252001},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.252001},
Abstract = {We report a measurement of the single-top-quark production
cross section in 2.2 fb-1 of pp̅ collision data
collected by the Collider Detector at Fermilab at
sqrt[s]=1.96 TeV. Candidate events are classified as
signal-like by three parallel analyses which use likelihood,
matrix element, and neural network discriminants. These
results are combined in order to improve the sensitivity. We
observe a signal consistent with the standard model
prediction, but inconsistent with the background-only model
by 3.7 standard deviations with a median expected
sensitivity of 4.9 standard deviations. We measure a cross
section of 2.2-0.6+0.7(stat+syst) pb, extract the
Cabibbo-Kobayashi-Maskawa matrix-element value
|Vtb|=0.88-0.12+0.13(stat+syst) ± 0.07(theory), and
set the limit |Vtb|>0.66 at the 95% C.L.},
Doi = {10.1103/physrevlett.101.252001},
Key = {fds308574}
}
@article{fds330935,
Author = {al, TAE},
Title = {Measurement of the Strong Coupling Constant from Inclusive
Jet Production at the Tevatron pb Collider},
Journal = {Physical Review Letters},
Volume = {88},
Number = {4},
Pages = {042001},
Year = {2002},
url = {http://dx.doi.org/10.1103/physrevlett.88.042001},
Abstract = {We report a measurement of the strong coupling constant,
alpha(s)(MZ), extracted from inclusive jet production in pp
collisions at square root[s] = 1800 GeV. The QCD prediction
for the evolution of alpha(s) with jet transverse energy ET
is tested over the range 40<ET<450 GeV using ET for the
renormalization scale. The data show good agreement with QCD
in the region below 250 GeV. The value of alpha(s) at the
mass of the Z0 boson averaged over the range 40<ET<250 GeV
is found to be alpha(s)(MZ) = 0.1178+/-0.0001(stat)+0.0081(-0.0095)(expt.
syst). The associated theoretical uncertainties are mainly
due to the choice of renormalization scale ((+6%)(-4%)) and
input parton distribution functions (5%).},
Doi = {10.1103/physrevlett.88.042001},
Key = {fds330935}
}
@article{fds308696,
Author = {Abulencia, and A, and others},
Title = {Measurement of the t anti-t production cross section in
$p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV in the all
hadronic decay mode},
Journal = {Phys. Rev.},
Volume = {D74},
Number = {7},
Pages = {072005},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.74.072005},
Abstract = {We report a measurement of the tt-bar production cross
section using the CDF II detector at the Fermilab Tevatron.
The analysis is performed using 322 pb-1 of p anti-p
collisions at s**(1/2) = 1.96 TeV. The data consist of
events selected with six or more hadronic jets with
additional kinematic requirements. At least one of these
jets must be identified as a b-quark jet by the
reconstruction of a secondary vertex. The cross section is
measured to be sigma_tt-bar = 7.5 +/- 2.1(stat.)+3.3_-2.2(syst.)+0.5_-0.4(lumi.)
pb, which is consistent with the standard model
prediction.},
Doi = {10.1103/PhysRevD.74.072005},
Key = {fds308696}
}
@article{fds308688,
Author = {Acosta, and D, and others},
Title = {Measurement of the t anti-t production cross section in p
anti-p collisions at sqrt[s]=1.96 TeV using lepton + jets
events with secondary vertex b-tagging},
Journal = {Phys. Rev.},
Volume = {D71},
Number = {7},
Pages = {052003},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.74.072006},
Abstract = {http://arxiv.org/abs/hep-ex/0410041},
Doi = {10.1103/PhysRevD.74.072006},
Key = {fds308688}
}
@article{fds365370,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling, JH},
Title = {Measurement of the t t¯ t t¯ production cross section in
pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2021)118},
Abstract = {A measurement of four-top-quark production using
proton-proton collision data at a centre-of-mass energy of
13 TeV collected by the ATLAS detector at the Large Hadron
Collider corresponding to an integrated luminosity of 139
fb−1 is presented. Events are selected if they contain a
single lepton (electron or muon) or an opposite-sign lepton
pair, in association with multiple jets. The events are
categorised according to the number of jets and how likely
these are to contain b-hadrons. A multivariate technique is
then used to discriminate between signal and background
events. The measured four-top-quark production cross section
is found to be 26−15+17 fb, with a corresponding observed
(expected) significance of 1.9 (1.0) standard deviations
over the background-only hypothesis. The result is combined
with the previous measurement performed by the ATLAS
Collaboration in the multilepton final state. The combined
four-top-quark production cross section is measured to be
24−6+7 fb, with a corresponding observed (expected) signal
significance of 4.7 (2.6) standard deviations over the
background-only predictions. It is consistent within 2.0
standard deviations with the Standard Model expectation of
12.0 ± 2.4 fb. [Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP11(2021)118},
Key = {fds365370}
}
@article{fds321249,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of the top pair production cross section in 8
TeV proton-proton collisions using kinematic information in
the lepton + jets final state with ATLAS},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.91.112013},
Abstract = {A measurement is presented of the (formula presented)
inclusive production cross section in pp collisions at a
center-of-mass energy of (formula presented) using data
collected by the ATLAS detector at the CERN Large Hadron
pffiffi Collider. The measurement was performed in the
lepton + jets final state using a data set corresponding to
an integrated luminosity of 20.3 fb-1. The cross section was
obtained using a likelihood discriminant fit and b-jet
identification was used to improve the signal-to-background
ratio. The inclusive tt production cross section was
measured to be (formula presented) pb assuming a top-quark
mass of 172.5 GeV, in good agreement with the theoretical
prediction of (formula presented) pb. The (formula
presented) production cross section in the fiducial region
determined by the detector acceptance is also
reported.},
Doi = {10.1103/PhysRevD.91.112013},
Key = {fds321249}
}
@article{fds308457,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of the top pair production cross section in the
$\mathrm{{lepton}}+\mathrm{{jets}}$ channel using a jet
flavor discriminant},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {3},
Pages = {031101},
Publisher = {American Physical Society},
Year = {2011},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.84.031101},
Abstract = {We present a new method to measure the top quark pair
production cross section and the background rates with data
corresponding to an integrated luminosity of 2.7fb-1 from
pp̄ collisions at √s=1.96TeV collected with the CDF II
Detector. We select events with a single electron or muon
candidate, missing transverse energy, and at least one
b-tagged jet. We perform a simultaneous fit to a jet flavor
discriminant across nine samples defined by the number of
jets and b tags. An advantage of this approach is that many
systematic uncertainties are measured in situ and inversely
scale with integrated luminosity. We measure a top cross
section of σ tt̄=7.64±0.57(stat+syst)±0.45(luminosity)pb.
© 2011 American Physical Society.},
Doi = {10.1103/PhysRevD.84.031101},
Key = {fds308457}
}
@article{fds308506,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the top pair production cross section in the
dilepton decay channel in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
collisions at $\sqrt{s}=1.96\,\,TeV$},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {5},
Pages = {052002},
Publisher = {American Physical Society},
Year = {2010},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.82.052002},
Abstract = {A measurement of the tt̄ production cross section in pp̄
collisions at √s=1.96TeV using events with two leptons,
missing transverse energy, and jets is reported. The data
were collected with the CDF II detector. The result in a
data sample corresponding to an integrated luminosity
2.8fb-1 is σtt̄=6.27±0.73(stat) ±0.63(syst)±0.39(lum)pb.
for an assumed top mass of 175GeV/c2. © 2010 The American
Physical Society.},
Doi = {10.1103/PhysRevD.82.052002},
Key = {fds308506}
}
@article{fds311479,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson,
TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand,
S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Measurement of the top quark charge in pp collisions at √s
= 7 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {11},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP11(2013)031},
Abstract = {A measurement of the top quark electric charge is carried
out in the ATLAS experiment at the Large Hadron Collider
using 2.05 fb-1 of data at a centre-of-mass energy of 7TeV.
In units of the elementary electric charge, the top quark
charge is determined to be 0.64 ± 0.02 (stat.) ± 0.08
(syst.) from the charges of the top quark decay products in
single lepton tt̄ candidate events. This excludes models
that propose a heavy quark of electric charge -4/3, instead
of the Standard Model top quark, with a significance of more
than 8σ. Copyright CERN.},
Doi = {10.1007/JHEP11(2013)031},
Key = {fds311479}
}
@article{fds308333,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Measurement of the top quark forward-backward production
asymmetry and its dependence on event kinematic
properties},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {9},
Pages = {092002},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.87.092002},
Abstract = {We present new measurements of the inclusive
forward-backward tt̄ production asymmetry, AFB, and its
dependence on several properties of the tt̄ system. The
measurements are performed with the full Tevatron data set
recorded with the CDF II detector during pp̄ collisions at
√s=1.96 TeV, corresponding to an integrated luminosity of
9.4 fb -1. We measure the asymmetry using the rapidity
difference Δy=yt-yt̄. Parton-level results are derived,
yielding an inclusive asymmetry of 0.164±0.047(stat+syst).
We establish an approximately linear dependence of AFB on
the top-quark pair mass Mtt̄ and the rapidity difference
|Δy| at detector and parton levels. Assuming the standard
model, the probabilities to observe the measured values or
larger for the detector-level dependencies are 7.4×10-3 and
2.2×10-3 for Mtt̄ and |Δy| respectively. Lastly, we study
the dependence of the asymmetry on the transverse momentum
of the tt̄ system at the detector level. These results are
consistent with previous lower-precision measurements and
provide additional quantification of the functional
dependencies of the asymmetry. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.87.092002},
Key = {fds308333}
}
@article{fds308496,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the Top Quark Mass and $p \bar{p} \to t
\bar{t}$ Cross Section in the All-Hadronic Mode with the
CDFII Detector},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {5},
Pages = {052011},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.052011},
Abstract = {http://arxiv.org/abs/1002.0365},
Doi = {10.1103/PhysRevD.81.052011},
Key = {fds308496}
}
@article{fds308832,
Author = {collaboration, CDF},
Title = {Measurement of the top quark mass and ${\rm t\bar{t}}$
production cross section from dilepton events at the
Collider Detector at Fermilab},
Journal = {Phys. Rev. Lett.},
Volume = {80},
Number = {2779},
Pages = {2767},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://arXiv.org/ps/hep-ex/9802017},
Abstract = {http://arXiv.org/ps/hep-ex/9802017},
Doi = {10.1103/PhysRevLett.80.2779},
Key = {fds308832}
}
@article{fds308556,
Author = {Aaltonen, T and others},
Title = {Measurement of the top quark mass at CDF using the
``neutrino phi weighting'' template method on a lepton plus
isolated track sample},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {7},
Pages = {072005},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.072005},
Abstract = {We present a measurement of the top quark mass with tt̄
dilepton events produced in pp̄ collisions at the Fermilab
Tevatron (s=1.96TeV) and collected by the CDF II detector. A
sample of 328 events with a charged electron or muon and an
isolated track, corresponding to an integrated luminosity of
2.9fb-1, are selected as tt̄ candidates. To account for the
unconstrained event kinematics, we scan over the phase space
of the azimuthal angles (ν1,ν2) of neutrinos and
reconstruct the top quark mass for each ν1, ν2 pair by
minimizing a χ2 function in the tt̄ dilepton hypothesis.
We assign χ2-dependent weights to the solutions in order to
build a preferred mass for each event. Preferred mass
distributions (templates) are built from simulated tt̄ and
background events, and parametrized in order to provide
continuous probability density functions. A likelihood fit
to the mass distribution in data as a weighted sum of signal
and background probability density functions gives a top
quark mass of 165.5-3.3+3.4(stat)±3. 1(syst)GeV/c2. © 2009
The American Physical Society.},
Doi = {10.1103/PhysRevD.79.072005},
Key = {fds308556}
}
@article{fds308641,
Author = {Abulencia, and A, and others},
Title = {Measurement of the Top Quark Mass in $p\bar{p}$Collisions at
$\sqrt{s} = 1.96$ TeV using the Decay Length
Technique},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {7},
Pages = {071102},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.071102},
Abstract = {We report the first measurement of the top quark mass using
the decay length technique in p[overline p] collisions at a
center-of-mass energy of 1.96 TeV. This technique uses the
measured flight distance of the b hadron to infer the mass
of the top quark in lepton plus jets events with missing
transverse energy. It relies solely on tracking and avoids
the jet energy scale uncertainty that is common to all other
methods used so far. We apply our novel method to a 695 pb-1
data sample recorded by the CDF II detector at Fermilab and
extract a measurement of mt=180.7-13.4+15.5(stat.)$\pm$8.6(syst.)
GeV/c2. While the uncertainty of this result is larger than
that of other measurements, the dominant uncertainties in
the decay length technique are uncorrelated with those in
other methods. This result can help reduce the overall
uncertainty when combined with other existing measurements
of the top quark mass.},
Doi = {10.1103/PhysRevD.75.071102},
Key = {fds308641}
}
@article{fds308419,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M},
Title = {Measurement of the top quark mass in the all-hadronic mode
at CDF},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {714},
Number = {1},
Pages = {24-31},
Publisher = {Elsevier BV},
Year = {2012},
Month = {July},
url = {http://dx.doi.org/10.1016/j.physletb.2012.06.007},
Abstract = {A measurement of the top quark mass (M top) in the
all-hadronic decay channel is presented. It uses 5.8 fb -1
of pp data collected with the CDF II detector at the
Fermilab Tevatron Collider. Events with six to eight jets
are selected by a neural network algorithm and by the
requirement that at least one of the jets is tagged as a
b-quark jet. The measurement is performed with a likelihood
fit technique, which simultaneously determines M top and the
jet energy scale (JES) calibration. The fit yields a value
of M top=172.5±1.4(stat)±1.0(JES)±1.1(syst) GeV/c 2. ©
2012 Elsevier B.V.},
Doi = {10.1016/j.physletb.2012.06.007},
Key = {fds308419}
}
@article{fds308461,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
Title = {Measurement of the top quark mass in the lepton+jets channel
using the lepton transverse momentum},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {698},
Number = {5},
Pages = {371-379},
Publisher = {Elsevier BV},
Year = {2011},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2011.03.041},
Abstract = {This Letter reports a measurement of the top quark mass,
Mtop, in data from pp- collisions at s=1.96 TeV
corresponding to 2.7 fb-1 of integrated luminosity at the
Fermilab Tevatron using the CDF II detector. Events with the
lepton+jets topology are selected. An unbinned likelihood is
constructed based on the dependence of the lepton transverse
momentum, PT, on Mtop. A maximum likelihood fit to the data
yields a measured mass Mtop=176.9±8.0stat±2.7syst GeV/c2.
In this measurement, the contribution by the jet energy
scale uncertainty to the systematic error is negligible. The
result provides an important consistency test for other Mtop
measurements where explicit use of the jet energy is made
for deriving the top quark mass. © 2011 Elsevier
B.V.},
Doi = {10.1016/j.physletb.2011.03.041},
Key = {fds308461}
}
@article{fds321208,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of the top quark mass in the tt¯→dilepton
channel from √s=8 TeV ATLAS data},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {761},
Pages = {350-371},
Publisher = {Elsevier BV},
Year = {2016},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2016.08.042},
Abstract = {The top quark mass is measured in the tt¯→dilepton
channel (lepton=e,μ) using ATLAS data recorded in the year
2012 at the LHC. The data were taken at a proton–proton
centre-of-mass energy of s=8 TeV and correspond to an
integrated luminosity of about 20.2 fb−1. Exploiting the
template method, and using the distribution of invariant
masses of lepton–b-jet pairs, the top quark mass is
measured to be mtop=172.99±0.41 (stat)±0.74 (syst) GeV,
with a total uncertainty of 0.84 GeV. Finally, a combination
with previous ATLAS mtop measurements from s=7 TeV data in
the tt¯→dilepton and tt¯→lepton+jets channels results
in mtop=172.84±0.34 (stat)±0.61 (syst) GeV, with a total
uncertainty of 0.70 GeV.},
Doi = {10.1016/j.physletb.2016.08.042},
Key = {fds321208}
}
@article{fds321302,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
Title = {Measurement of the top quark mass in the [Formula: see text]
and [Formula: see text] channels using [Formula: see
text] [Formula: see text] ATLAS data.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {330},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3544-0},
Doi = {10.1140/epjc/s10052-015-3544-0},
Key = {fds321302}
}
@article{fds308692,
Author = {Abulencia, and A, and others},
Title = {Measurement of the top quark mass using template methods on
dilepton events in proton antiproton collisions at $\sqrt{s}
=$ 1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {11},
Pages = {112006},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.73.112006},
Abstract = {We describe a measurement of the top quark mass from events
produced in p anti-p collisions at a center-of-mass energy
of 1.96 TeV, using the Collider Detector at Fermilab. We
identify tt-bar candidates where both W bosons from the top
quarks decay into leptons (e mu, mu nu, or tau nu) from a
data sample of 360 pb-1. The top quark mass is reconstructed
in each event separately by three different methods, which
draw upon simulated distributions of the neutrino
pseudorapi+dity, tt-bar longitudinal momentum, or neutrino
azimuthal angle in order to extract probability
distributions for the top quark mass. For each method,
representative mass distributions, or templates, are
constructed from simulated samples of signal and background
events, and parametrized templates is then performed on the
data sample masses in order to derive a final top quark
mass. Combining the three template methods, taking into
account correlations in their statistical and systematic
uncertainties, results in a top quark mass measurement of
170.1 +/- 6.0 (stat.) +/- 4.1 (syst.) GeV/c2.},
Doi = {10.1103/PhysRevD.73.112006},
Key = {fds308692}
}
@article{fds308557,
Author = {Aaltonen, T and others},
Title = {Measurement of the top quark mass using the invariant mass
of lepton pairs in soft muon b-tagged events},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {5},
Pages = {051104},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.051104},
Abstract = {We present the first measurement of the mass of the top
quark in a sample of tt̅ →ℓν̅ bb̅ qq̅ events (where
ℓ=e,μ) selected by identifying jets containing a muon
candidate from the semileptonic decay of heavy-flavor
hadrons (soft muon b tagging). The pp̅ collision data used
correspond to an integrated luminosity of 2 fb-1 and
were collected by the CDF II detector at the Fermilab
Tevatron Collider. The measurement is based on a novel
technique exploiting the invariant mass of a subset of the
decay particles, specifically the lepton from the W boson of
the t→Wb decay and the muon from a semileptonic b decay.
We fit template histograms, derived from simulation of tt̅
events and a modeling of the background, to the mass
distribution observed in the data and measure a top quark
mass of 180.5 ± 12.0(stat) ±
3.6(syst) GeV/c2, consistent with the current world
average value.},
Doi = {10.1103/PhysRevD.80.051104},
Key = {fds308557}
}
@article{fds331231,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and P. De Barbaro and PDB and Barbaro-Galtieri, AG and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers,
W and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Culbertson, R and Dagenhart, D and Daniels, T and De Jongh and F and Dell’agnello, S and Dell’orso, M},
Title = {Measurement of the top quark mass with the collider detector
at fermilab},
Journal = {Physical Review Letters},
Volume = {82},
Number = {2},
Pages = {271-276},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.271},
Abstract = {We present a new measurement of the top quark mass in tt
events in which both W bosons from top quarks decay into
leptons (e ν, μ ν). We use events collected by the CDF
experiment from pp collisions at √ s=1.8 TeV at the
Tevatron collider. We measure a top quark mass of 167.4 ±
10.3 (stat) ± 4.8 (syst) GeV/c2 from a sample of eight
events. We combine this result with previous CDF
measurements in other decay channels to obtain a final mass
value of 176.0 ± 6.5 GeV/c2. © 2000 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.82.271},
Key = {fds331231}
}
@article{fds308806,
Author = {collaboration, CDF},
Title = {Measurement of the top quark mass with the Collider Detector
at Fermilab},
Journal = {Phys.Rev. Lett.},
Volume = {82},
Number = {271},
Year = {1999},
Month = {January},
url = {http://arXiv.org/ps/hep-ex/9810029},
Abstract = {http://arXiv.org/ps/hep-ex/9810029},
Key = {fds308806}
}
@article{fds308681,
Author = {Abulencia, and A, and others},
Title = {Measurement of the top quark mass with the dynamical
likelihood method using lepton plus jets events with b-tags
in $p\bar{p}$ collisions at $\sqrt{s} =$
1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {9},
Pages = {092002},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.73.092002},
Abstract = {This report describes a measurement of the top quark mass,
M_top, with the dynamical likelihood method (DLM) using the
CDF II detector at the Fermilab Tevatron. The Tevatron
produces top/anti-top (t anti-t) pairs in p anti-p
collisions at a center-of-mass energy of 1.96 TeV. The data
sample used in this analysis was accumulated from March 2002
through August 2004, which corresponds to an integrated
luminosity of 318 pb-1. We use the tt-bar candidates in the
``epton+jets'' decay channel, requiring at least one jet
identified as a b quark by finding a displaced secondary
vertex. The DLM defines a likelihood for each event based on
the differential cross section s a function of M_top per
unit phase space volume of the final partons, multiplied by
the transfer functions from jet to parton energies. The
method takes into account all possible jet combinations in
an event, and the likelihood is multiplied event by event to
derive the top quark mass by the maximum likelihood method.
Using 63 tt-bar candidates observed in the data, with 9.2
events expected from background, we measure the top quark
mass to be 173.2+2.6_-2.4 (stat.) +/- 3.2 (syst.) GeV/c2, or
173+4.1_-4.0 GeV/c2.},
Doi = {10.1103/PhysRevD.73.092002},
Key = {fds308681}
}
@article{fds308286,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
S},
Title = {Measurement of the top quark pair production charge
asymmetry in proton-proton collisions at √s = 7 TeV using
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {2},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP02(2014)107},
Abstract = {This paper presents a measurement of the top quark pair
(tt̄) production charge asymmetry AC using 4.7 fb-1 of
proton-proton collisions at a centre-of-mass energy √s =
7TeV collected by the ATLAS detector at the LHC. A
tt̄-enriched sample of events with a single lepton
(electron or muon), missing transverse momentum and at least
four high transverse momentum jets, of which at least one is
tagged as coming from a b-quark, is selected. A likelihood
fit is used to reconstruct the tt̄ event kinematics. A
Bayesian unfolding procedure is employed to estimate AC at
the parton-level. The measured value of the tt̄ production
charge asymmetry is AC = 0.006 ± 0.010, where the
uncertainty includes both the statistical and the systematic
components. Differential AC measurements as a function of
the invariant mass, the rapidity and the transverse momentum
of the tt̄- system are also presented. In addition, AC is
measured for a subset of events with large tt̄ velocity,
where physics beyond the Standard Model could contribute.
All measurements are consistent with the Standard Model
predictions.},
Doi = {10.1007/JHEP02(2014)107},
Key = {fds308286}
}
@article{fds308629,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the top-quark mass in all-hadronic decays in
p anti-p collisions at CDF II},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {14},
Pages = {142001},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.142001},
Abstract = {We present a measurement of the top-quark mass Mtop in the
all-hadronic decay channel t[overline t]-->W+bW-[overline
b]-->q1[overline q]2bq3[overline q]4[overline b]. The
analysis is performed using 310 pb-1 of sqrt(s)=1.96 TeV
p[overline p] collisions collected with the CDF II detector
using a multijet trigger. The mass measurement is based on
an event-by-event likelihood which depends on both the
sample purity and the value of the top-quark mass, using 90
possible jet-to-parton assignments in the six-jet final
state. The joint likelihood of 290 selected events yields a
value of Mtop=177.1$\pm$4.9(stat)$\pm$4.7(syst)
GeV/c2.},
Doi = {10.1103/physrevlett.98.142001},
Key = {fds308629}
}
@article{fds321316,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of the top-quark mass in the all-hadronic
channel using the full CDF data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.90.091101},
Abstract = {The top-quark mass Mtop is measured using top
quark-antiquark pairs produced in proton-antiproton
collisions at a center-of-mass energy of 1.96 TeV and that
decay into a fully hadronic final state. The full data set
collected with the CDF II detector at the Fermilab Tevatron
Collider, corresponding to an integrated luminosity of
9.3fb-1, is used. Events are selected that have six to eight
jets, at least one of which is identified as having
originated from a b quark. In addition, a multivariate
algorithm, containing multiple kinematic variables as
inputs, is used to discriminate signal events from
background events due to QCD multijet production. Templates
for the reconstructed top-quark mass are combined in a
likelihood fit to measure Mtop with a simultaneous
calibration of the jet energy scale. A value of
Mtop=175.07±1.19(stat)-1.58+1.55(syst)GeV/c2 is obtained
for the top-quark mass.},
Doi = {10.1103/PhysRevD.90.091101},
Key = {fds321316}
}
@article{fds321295,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin,
V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
A},
Title = {Measurement of the top-quark mass in the fully hadronic
decay channel from ATLAS data at [Formula: see
text].},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {4},
Pages = {158},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3373-1},
Abstract = {The mass of the top quark is measured in a data set
corresponding to 4.6 [Formula: see text] of proton-proton
collisions with centre-of-mass energy [Formula: see
text] TeV collected by the ATLAS detector at the LHC.
Events consistent with hadronic decays of top-antitop quark
pairs with at least six jets in the final state are
selected. The substantial background from multijet
production is modelled with data-driven methods that utilise
the number of identified [Formula: see text]-quark jets and
the transverse momentum of the sixth leading jet, which have
minimal correlation. The top-quark mass is obtained from
template fits to the ratio of three-jet to dijet mass. The
three-jet mass is calculated from the three jets produced in
a top-quark decay. Using these three jets the dijet mass is
obtained from the two jets produced in the [Formula: see
text] boson decay. The top-quark mass obtained from this fit
is thus less sensitive to the uncertainty in the energy
measurement of the jets. A binned likelihood fit yields a
top-quark mass of [Formula: see text].},
Doi = {10.1140/epjc/s10052-015-3373-1},
Key = {fds321295}
}
@article{fds308446,
Author = {Aaltonen, TEA},
Title = {Measurement of the top-quark mass in the lepton+jets channel
using a matrix element technique with the {CDF II}
detector},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {7},
Pages = {071105},
Publisher = {American Physical Society},
Year = {2011},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.84.071105},
Abstract = {A measurement of the top-quark mass is presented using
Tevatron data from proton-antiproton collisions at
center-of-mass energy √s=1.96TeV collected with the CDF II
detector. Events are selected from a sample of candidates
for production of tt̄ pairs that decay into the lepton+jets
channel. The top-quark mass is measured with an unbinned
maximum likelihood method where the event probability
density functions are calculated using signal and background
matrix elements, as well as a set of parametrized
jet-to-parton transfer functions. The likelihood function is
maximized with respect to the top-quark mass, the signal
fraction in the sample, and a correction to the jet energy
scale (JES) calibration of the calorimeter jets. The
simultaneous measurement of the JES correction (ΔJES)
amounts to an additional in situ jet energy calibration
based on the known mass of the hadronically decaying W
boson. Using the data sample of 578 lepton+jets candidate
events, corresponding to 3.2fb-1 of integrated luminosity,
the top-quark mass is measured to be mt=172.4±1.4(stat+ΔJES)±1.
3(syst)GeV/c2. © 2011 American Physical
Society.},
Doi = {10.1103/PhysRevD.84.071105},
Key = {fds308446}
}
@article{fds321231,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of the top-quark mass in the tt¯ dilepton
channel using the full CDF Run II data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.92.032003},
Abstract = {We present a measurement of the top-quark mass in events
containing two leptons (electrons or muons) with a large
transverse momentum, two or more energetic jets, and a
transverse-momentum imbalance. We use the full
proton-antiproton collision data set collected by the CDF
experiment during the Fermilab Tevatron Run II at
center-of-mass energy s=1.96 TeV, corresponding to an
integrated luminosity of 9.1 fb-1. A special observable is
exploited for an optimal reduction of the dominant
systematic uncertainty, associated with the knowledge of the
absolute energy of the hadronic jets. The distribution of
this observable in the selected events is compared to
simulated distributions of tt¯ dilepton signal and
background. We measure a value for the top-quark mass of
171.5±1.9 (stat)±2.5 (syst) GeV/c2.},
Doi = {10.1103/PhysRevD.92.032003},
Key = {fds321231}
}
@article{fds308634,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the top-quark mass using missing $E_T$ + jets
events with secondary vertex $b-$tagging at CDF
II},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {11},
Pages = {111103},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.111103},
Abstract = {We present a measurement of the top-quark mass in p[overline
p] collisions at sqrt(s)=1.96 TeV which uses events with an
inclusive signature of missing transverse energy and jets.
The event selection is sensitive to t[overline
t]-->W+bW-[overline b]-->lnubqq[prime][overline b]
independent of the lepton flavor and results in a large
acceptance for W-->taunu decays. All-hadronic t[overline t]
decays and events with identified electrons or muons are
vetoed to provide a statistically independent sample with
respect to all previous measurements. The top-quark mass is
inferred from the distribution of the scalar sum of all jet
transverse energies and the missing transverse energy. Using
311 pb-1 of integrated luminosity recorded by the Collider
Detector at Fermilab, we measure a top-quark mass
mt=172.3-9.6+10.8(stat)$\pm$10.8(syst) GeV/c2. While the
uncertainty on mt is larger than that of other measurements,
the result is statistically uncorrelated with those of other
methods and thus can help to reduce the overall mt
uncertainty when combined with other existing
measurements.},
Doi = {10.1103/PhysRevD.75.111103},
Key = {fds308634}
}
@article{fds308528,
Author = {Aaltonen, T and others},
Title = {Measurement of the Top-Quark Mass with Dilepton Events
Selected Using Neuroevolution at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {15},
Pages = {152001},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.152001},
Abstract = {We present an analysis of the mass of the X(3872)
reconstructed via its decay to J/ψπ+π- using
2.4 fb-1 of integrated luminosity from pp̅ collisions
at sqrt[s]=1.96 TeV, collected with the CDF II detector
at the Fermilab Tevatron. The possible existence of two
nearby mass states is investigated. Within the limits of our
experimental resolution the data are consistent with a
single state, and having no evidence for two states we set
upper limits on the mass difference between two hypothetical
states for different assumed ratios of contributions to the
observed peak. For equal contributions, the 95% confidence
level upper limit on the mass difference is 3.6 MeV/c2.
Under the single-state model the X(3872) mass is measured to
be 3871.61$\pm$0.16(stat)$\pm$0.19(syst) MeV/c2, which
is the most precise determination to date.},
Doi = {10.1103/physrevlett.102.152001},
Key = {fds308528}
}
@article{fds308298,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Measurement of the top-quark pair-production cross section
in events with two leptons and bottom-quark jets using the
full CDF data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.88.091103},
Abstract = {We present a measurement of the top-quark pair production
cross section in proton-antiproton collisions at √s=1.96
TeV. The data were collected at the Fermilab Tevatron by the
CDF II detector and correspond to an integrated luminosity
of 8.8 fb-1, representing the complete CDF Run II data set.
We select events consistent with the production of top-quark
pairs by requiring the presence of two reconstructed
leptons, an imbalance in the total event transverse
momentum, and jets. At least one jet is required to be
identified as consistent with the fragmentation of a bottom
quark using a secondary-vertex-finding algorithm. The 246
candidate events are estimated to have a signal purity of
91%. We measure a cross section of σ tt̄=7.09±0.84 pb,
assuming a top-quark mass of 172.5 GeV/c2. The results are
consistent with the standard model as predicted by
next-to-leading-order calculations. Published by the
American Physical Society.},
Doi = {10.1103/PhysRevD.88.091103},
Key = {fds308298}
}
@article{fds375950,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
Ferraz, V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Measurement of the total cross section and ρ -parameter
from elastic scattering in pp collisions at √s=13 TeV with
the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11436-8},
Abstract = {In a special run of the LHC with β⋆= 2.5 km,
proton–proton elastic-scattering events were recorded at
s=13 TeV with an integrated luminosity of 340μb-1 using the
ALFA subdetector of ATLAS in 2016. The elastic cross section
was measured differentially in the Mandelstam t variable in
the range from - t= 2.5 · 10 - 4 GeV 2 to - t= 0.46 GeV 2
using 6.9 million elastic-scattering candidates. This paper
presents measurements of the total cross section σtot ,
parameters of the nuclear slope, and the ρ -parameter
defined as the ratio of the real part to the imaginary part
of the elastic-scattering amplitude in the limit t→ 0 .
These parameters are determined from a fit to the
differential elastic cross section using the optical theorem
and different parameterizations of the t-dependence. The
results for σtot and ρ are σtot(pp→X)=104.7±1.1mb,ρ=0.098±0.011.
The uncertainty in σtot is dominated by the luminosity
measurement, and in ρ by imperfect knowledge of the
detector alignment and by modelling of the nuclear
amplitude.},
Doi = {10.1140/epjc/s10052-023-11436-8},
Key = {fds375950}
}
@article{fds314174,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurement of the total cross section from elastic
scattering in pp collisions at √s=7 TeV with the ATLAS
detector},
Journal = {Nuclear Physics B},
Volume = {889},
Pages = {486-548},
Publisher = {Elsevier BV},
Year = {2014},
Month = {December},
ISSN = {0550-3213},
url = {http://dx.doi.org/10.1016/j.nuclphysb.2014.10.019},
Abstract = {A measurement of the total pp cross section at the LHC at
s=7 TeV is presented. In a special run with high-β⋆ beam
optics, an integrated luminosity of 80 μb−1 was
accumulated in order to measure the differential elastic
cross section as a function of the Mandelstam momentum
transfer variable t. The measurement is performed with the
ALFA sub-detector of ATLAS. Using a fit to the differential
elastic cross section in the |t| range from 0.01 GeV2 to 0.1
GeV2 to extrapolate to |t|→0, the total cross section,
σtot(pp→X), is measured via the optical theorem to be:
σtot(pp→X)=95.35±0.38(stat.)±1.25(exp.)±0.37(extr.)mb,
where the first error is statistical, the second accounts
for all experimental systematic uncertainties and the last
is related to uncertainties in the extrapolation to |t|→0.
In addition, the slope of the elastic cross section at small
|t| is determined to be B=19.73±0.14(stat.)±0.26(syst.)
GeV−2.},
Doi = {10.1016/j.nuclphysb.2014.10.019},
Key = {fds314174}
}
@article{fds321154,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of the total cross section from elastic
scattering in pp collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {761},
Pages = {158-178},
Publisher = {Elsevier BV},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2016.08.020},
Abstract = {A measurement of the total pp cross section at the LHC at
s=8 TeV is presented. An integrated luminosity of 500
μb−1 was accumulated in a special run with high-β⋆
beam optics to measure the differential elastic cross
section as a function of the Mandelstam momentum transfer
variable t. The measurement is performed with the ALFA
sub-detector of ATLAS. Using a fit to the differential
elastic cross section in the −t range from 0.014 GeV2 to
0.1 GeV2 to extrapolate t→0, the total cross section,
σtot(pp→X), is measured via the optical theorem to be
σtot(pp→X)=96.07±0.18(stat.)±0.85(exp.)±0.31(extr.)mb,
where the first error is statistical, the second accounts
for all experimental systematic uncertainties and the last
is related to uncertainties in the extrapolation t→0. In
addition, the slope of the exponential function describing
the elastic cross section at small t is determined to be
B=19.74±0.05(stat.)±0.23(syst.)GeV−2.},
Doi = {10.1016/j.physletb.2016.08.020},
Key = {fds321154}
}
@article{fds316859,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
Title = {Measurement of the transverse momentum and [Formula: see
text] distributions of Drell-Yan lepton pairs in
proton-proton collisions at [Formula: see text] TeV with
the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {291},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4070-4},
Abstract = {Distributions of transverse momentum [Formula: see text] and
the related angular variable [Formula: see text] of
DrellΓÇôYan lepton pairs are measured in
20.3 fb[Formula: see text] of proton–proton
collisions at [Formula: see text] TeV with the ATLAS
detector at the LHC. Measurements in electron-pair and
muon-pair final states are corrected for detector effects
and combined. Compared to previous measurements in
protonΓÇôproton collisions at [Formula: see
text] TeV, these new measurements benefit from a larger
data sample and improved control of systematic
uncertainties. Measurements are performed in bins of
lepton-pair mass above, around and below the <i>Z</i>-boson
mass peak. The data are compared to predictions from
perturbative and resummed QCD calculations. For values of
[Formula: see text] the predictions from the Monte Carlo
generator ResBos are generally consistent with the data
within the theoretical uncertainties. However, at larger
values of [Formula: see text] this is not the case. Monte
Carlo generators based on the parton-shower approach are
unable to describe the data over the full range of [Formula:
see text] while the fixed-order prediction of Dynnlo falls
below the data at high values of [Formula: see text]. ResBos
and the parton-shower Monte Carlo generators provide a much
better description of the evolution of the [Formula: see
text] and [Formula: see text] distributions as a function of
lepton-pair mass and rapidity than the basic shape of the
data.},
Doi = {10.1140/epjc/s10052-016-4070-4},
Key = {fds316859}
}
@article{fds321270,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of the transverse polarization of Λ and Λ ¯
hyperons produced in proton-proton collisions at √s = 7
TeV using the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.91.032004},
Abstract = {The transverse polarization of Λ and Λ¯ hyperons produced
in proton-proton collisions at a center-of-mass energy of 7
TeV is measured. The analysis uses 760 μb-1 of minimum bias
data collected by the ATLAS detector at the LHC in the year
2010. The measured transverse polarization averaged over
Feynman xF from 5×10-5 to 0.01 and transverse momentum pT
from 0.8 to 15 GeV is -0.010±0.005(stat)±0.004(syst) for
Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. It is also
measured as a function of xF and pT, but no significant
dependence on these variables is observed. Prior to this
measurement, the polarization was measured at fixed-target
experiments with center-of-mass energies up to about 40 GeV.
The ATLAS results are compatible with the extrapolation of a
fit from previous measurements to the xF range covered by
this measurement.},
Doi = {10.1103/PhysRevD.91.032004},
Key = {fds321270}
}
@article{fds308731,
Author = {al, DAE},
Title = {Measurement of the tt-bar Production Cross Section in pp-bar
Collisions at sqrt[s]=1.96 TeV Using Dilepton
Events},
Journal = {Physical Review Letters},
Volume = {93},
Number = {14},
Pages = {142001},
Year = {2004},
Month = {October},
url = {http://www-cdf.fnal.gov/physics/preprints/cdf6882_top_dil_200pb_v7.ps},
Abstract = {We report a measurement of the tt-bar production cross
section using dilepton events with jets and missing
transverse energy in pp-bar collisions at a center-of- mass
energy of 1.96 TeV. Using a 197±12 pb-1 data sample
recorded by the upgraded Collider Detector at Fermilab, we
use two complementary techniques to select candidate events.
We compare the number of observed events and selected
kinematical distributions with the predictions of the
standard model and find good agreement. The combined result
of the two techniques yields a tt-bar production cross
section of 7.0+2.4 -2.1(stat)+1.6-1.1(syst)±0.4(lum)
pb.},
Doi = {10.1103/physrevlett.93.142001},
Key = {fds308731}
}
@article{fds375878,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Aktas, S and Al Khoury and K and Alberghi,
GL and Albert, J and Albicocco, P and Albouy, GL and Alderweireldt, S and Alegria, ZL and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Measurement of the tt¯ cross section and its ratio to the Z
production cross section using pp collisions at s=13.6 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {848},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138376},
Abstract = {The inclusive top-quark-pair production cross section σtt¯
and its ratio to the Z-boson production cross section have
been measured in proton–proton collisions at s=13.6 TeV,
using 29 fb−1 of data collected in 2022 with the ATLAS
experiment at the Large Hadron Collider. Using events with
an opposite-charge electron-muon pair and b-tagged jets, and
assuming Standard Model decays, the top-quark-pair
production cross section is measured to be
σtt¯=850±3(stat.)±18(syst.)±20(lumi.) pb. The ratio of
the tt¯ and the Z-boson production cross sections is also
measured, where the Z-boson contribution is determined for
inclusive e+e− and μ+μ− events in a fiducial phase
space. The relative uncertainty on the ratio is reduced
compared to the tt¯ cross section, thanks to the
cancellation of several systematic uncertainties. The result
for the ratio, Rtt¯/Z=1.145±0.003(stat.)±0.021(syst.)±0.002(lumi.)
is consistent with the Standard Model prediction using the
PDF4LHC21 PDF set.},
Doi = {10.1016/j.physletb.2023.138376},
Key = {fds375878}
}
@article{fds321282,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the tt¯ production cross-section as a
function of jet multiplicity and jet transverse momentum in
7 TeV proton-proton collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {1},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2015)020},
Abstract = {Abstract: The tt¯$$ t\overline{t} $$ production
cross-section dependence on jet multiplicity and jet
transverse momentum is reported for proton-proton collisions
at a centre-of-mass energy of 7 TeV in the single-lepton
channel. The data were collected with the ATLAS detector at
the CERN Large Hadron Collider and comprise the full 2011
data sample corresponding to an integrated luminosity of 4.6
fb−1. Differential cross-sections are presented as a
function of the jet multiplicity for up to eight jets using
jet transverse momentum thresholds of 25, 40, 60, and 80
GeV, and as a function of jet transverse momentum up to the
fifth jet. The results are shown after background
subtraction and corrections for all known detector effects,
within a kinematic range closely matched to the experimental
acceptance. Several QCD-based Monte Carlo models are
compared with the results. Sensitivity to the parton shower
modelling is found at the higher jet multiplicities, at high
transverse momentum of the leading jet and in the transverse
momentum spectrum of the fifth leading jet. The
MC@NLO+HERWIG MC is found to predict too few events at
higher jet multiplicities.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP01(2015)020},
Key = {fds321282}
}
@article{fds321207,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of the tt¯ production cross-section using eμ
events with b-tagged jets in pp collisions at √s=13TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {761},
Pages = {136-157},
Publisher = {Elsevier BV},
Year = {2016},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2016.08.019},
Abstract = {This paper describes a measurement of the inclusive top
quark pair production cross-section (σtt¯) with a data
sample of 3.2fb−1 of proton–proton collisions at a
centre-of-mass energy of s=13TeV, collected in 2015 by the
ATLAS detector at the LHC. This measurement uses events with
an opposite-charge electron–muon pair in the final state.
Jets containing b-quarks are tagged using an algorithm based
on track impact parameters and reconstructed secondary
vertices. The numbers of events with exactly one and exactly
two b-tagged jets are counted and used to determine
simultaneously σtt¯ and the efficiency to reconstruct and
b-tag a jet from a top quark decay, thereby minimising the
associated systematic uncertainties. The cross-section is
measured to be: σtt¯=818±8(stat)±27(syst)±19(lumi)±12(beam)
pb, where the four uncertainties arise from data statistics,
experimental and theoretical systematic effects, the
integrated luminosity and the LHC beam energy, giving a
total relative uncertainty of 4.4%. The result is consistent
with theoretical QCD calculations at next-to-next-to-leading
order. A fiducial measurement corresponding to the
experimental acceptance of the leptons is also
presented.},
Doi = {10.1016/j.physletb.2016.08.019},
Key = {fds321207}
}
@article{fds314162,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canelli, F and Canepa, A and Casarsa, M and Carlsmith, D and Carosi,
R and Carron, S and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chou, JP and Chuang, S and Chung, K and Chung, WH and Chung, YS and Cijliak, M and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Cruz, A and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Demers,
S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and Dituro, P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
JP and Field, RD and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii,
Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grosso-Pilcher, C and Grundler, U and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
N and Miles, J and Miller, L and Miller, R and Miller, JS and Mills, C and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi,
N and Mohr, B and Moore, R and Morello, M and Fernandez, PAM and Muelmenstaedt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Nelson, T and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Ohsugi,
T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Osterberg,
K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou,
V and Paramonov, AA and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo,
T and Rolli, S and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis,
RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sill, A and Sinervo, P and Sisakyan, A and Sjolin, J and Skiba, A and Slaughter, AJ and Sliwa,
K},
Title = {Measurement of the tt̄ production cross section in pp̄
collisions at s=1.96 TeV using lepton plus jets events with
semileptonic B decays to muons},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {72},
Number = {3},
Pages = {1-20},
Publisher = {American Physical Society (APS)},
Year = {2005},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.72.032002},
Abstract = {We present a measurement of the tt̄ production cross
section using 194 pb-1 of CDF II data using events with a
high transverse momentum electron or muon, three or more
jets, and missing transverse energy. The measurement assumes
100% t→Wb branching fraction. Events consistent with tt̄
decay are found by identifying jets containing heavy-flavor
semileptonic decays to muons. The dominant backgrounds are
evaluated directly from the data. Based on 20 candidate
events and an expected background of 9.5±1.1 events, we
measure a production cross section of 5.3±3.3-1.0+1.3 pb,
in agreement with the standard model. © 2005 The American
Physical Society.},
Doi = {10.1103/PhysRevD.72.032002},
Key = {fds314162}
}
@article{fds308713,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery,
M},
Title = {Measurement of the tt̄ production cross section in pp̄
collisions at √s = 1.96 TeV using lepton + jets events
with secondary vertex b -tagging},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {5},
Pages = {1-28},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.71.052003},
Abstract = {We present a measurement of the tt̄ production cross
section using events with one charged lepton and jets from
pp̄ collisions at a center-of-mass energy of 1.96 TeV. In
these events, heavy flavor quarks from top quark decay are
identified with a secondary vertex tagging algorithm. From
162 pb<sup>-1</sup> of data collected by the Collider
Detector at Fermilab, a total of 48 candidate events are
selected, where 13.5 ± 1.8 events are expected from
background contributions. We measure a tt̄ production cross
section of 5.6<inf>-1.1</inf><sup>+1.2</sup>(stat.)<inf>-0.6</inf><sup>+0.9</sup>(syst.)
pb. © 2005 The American Physical Society.},
Doi = {10.1103/PhysRevD.71.052003},
Key = {fds308713}
}
@article{fds314165,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli,
M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron,
S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen,
C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang,
S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker,
GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, J and Frisch,
H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko,
S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko,
I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann,
SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefevre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel,
P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller,
T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu,
C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov,
T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh,
SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn,
F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno,
M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet,
M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba,
A},
Title = {Measurement of the tt̄ production cross section in pp̄
collisions at √s=1:96 TeV using kinematic fitting of
b-tagged lepton+jet events},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {7},
Pages = {1-11},
Publisher = {American Physical Society (APS)},
Year = {2005},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.71.072005},
Abstract = {We report a measurement of the tt̄ production cross section
using the CDF II detector at the Fermilab Tevatron. The data
consist of events with an energetic electron or muon,
missing transverse energy, and three or more hadronic jets,
at least one of which is identified as a b-quark jet by
reconstructing a secondary vertex. The background fraction
is determined from a fit of the transverse energy of the
leading jet. Using 162 ± 10 pb -1 of data, the total cross
section is found to be 6.0 ± 1.6(stat.) ± 1.2(syst.) pb,
which is consistent with the standard model prediction. ©
2005 The American Physical Society.},
Doi = {10.1103/PhysRevD.71.072005},
Key = {fds314165}
}
@article{fds308563,
Author = {Aaltonen, T and others},
Title = {Measurement of the tt̅ cross section in pp̅ collisions at
sqrt[s] =1.96 TeV using dilepton events with a lepton plus
track selection},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {11},
Pages = {112007},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.112007},
Abstract = {This paper reports a measurement of the cross section for
the pair production of top quarks in pp̅ collisions at
sqrt[s]=1.96 TeV at the Fermilab Tevatron. The data
were collected from the CDF run II detector in a set of runs
with a total integrated luminosity of 1.1 fb-1. The
cross section is measured in the dilepton channel, the
subset of tt̅ events in which both top quarks decay through
t→Wb→ℓνb, where ℓ=e, μ, or τ. The lepton pair is
reconstructed as one identified electron or muon and one
isolated track. The use of an isolated track to identify the
second lepton increases the tt̅ acceptance, particularly
for the case in which one W decays as W→τν. The purity
of the sample may be further improved at the cost of a
reduction in the number of signal events, by requiring an
identified b jet. We present the results of measurements
performed with and without the request of an identified b
jet. The former is the first published CDF result for which
a b-jet requirement is added to the dilepton selection. In
the CDF data there are 129 pretag lepton+track candidate
events, of which 69 are tagged. With the tagging
information, the sample is divided into tagged and untagged
subsamples, and a combined cross section is calculated by
maximizing a likelihood. The result is σtt̅ =9.6 ±
1.2(stat)-0.5+0.6(sys) ± 0.6(lum) pb, assuming a
branching ratio of BR(W→ℓν)=10.8% and a top mass of
mt=175 GeV/c2.},
Doi = {10.1103/PhysRevD.79.112007},
Key = {fds308563}
}
@article{fds308554,
Author = {Aaltonen, T and others},
Title = {Measurement of the t[overline t] production cross section in
2 fb[sup -1] of p[overline p] collisions at sqrt(s) = 1.96
TeV using lepton plus jets events with soft muon b
tagging},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {5},
Pages = {052007},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.052007},
Abstract = {We present a measurement of the tt̄ production cross
section in pp̄ collisions at s=1.96TeV using events
containing a high transverse momentum electron or muon,
three or more jets, and missing transverse energy. Events
consistent with tt̄ decay are found by identifying jets
containing candidate heavy-flavor semileptonic decays to
muons. The measurement uses a CDF run II data sample
corresponding to 2fb-1 of integrated luminosity. Based on
248 candidate events with three or more jets and an expected
background of 79.5±5.3 events, we measure a production
cross section of 9.1±1.6pb. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevD.79.052007},
Key = {fds308554}
}
@article{fds308844,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and De Barbaro and P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari,
C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti,
R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers,
W and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and De Jongh and F and Dell’agnello, S and Dell’orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF},
Title = {Measurement of the t¯t Production Cross Section in p¯p
Collisions at √s = 1.8TeV},
Journal = {Physical Review Letters},
Volume = {80},
Number = {13},
Pages = {2773-2778},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.2773},
Abstract = {We present a measurement of the t¯t production cross
section in p¯p collisions at √s = 1.8TeV using an
integrated luminosity of 109pb-1 collected with the Collider
Detector at Fermilab. The measurement uses t¯t decays into
final states which contain one or two high transverse
momentum leptons and multiple jets, and final states which
contain only jets. Using acceptances appropriate for a top
quark mass of 175GeV/c2, we find σt¯t = 7.6+1.8-1.5pb. ©
1998 The American Physical Society.},
Doi = {10.1103/PhysRevLett.80.2773},
Key = {fds308844}
}
@article{fds321341,
Author = {The ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa,
C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung,
C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso,
S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Measurement of the underlying event in jet events from
7 TeV proton–proton collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {74},
Number = {8},
Pages = {1-29},
Publisher = {Springer Nature},
Year = {2014},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-2965-5},
Abstract = {Distributions sensitive to the underlying event in QCD jet
events have been measured with the ATLAS detector at the
LHC, based on (Formula presented.) of proton–proton
collision data collected at a centre-of-mass energy of
7 (Formula presented.). Charged-particle mean (Formula
presented.) and densities of all-particle (Formula
presented.) and charged-particle multiplicity and (Formula
presented.) have been measured in regions azimuthally
transverse to the hardest jet in each event. These are
presented both as one-dimensional distributions and with
their mean values as functions of the leading-jet transverse
momentum from 20 to 800 (Formula presented.). The
correlation of charged-particle mean (Formula presented.)
with charged-particle multiplicity is also studied, and the
(Formula presented.) densities include the forward rapidity
region; these features provide extra data constraints for
Monte Carlo modelling of colour reconnection and
beam-remnant effects respectively. For the first time,
underlying event observables have been computed separately
for inclusive jet and exclusive dijet event selections,
allowing more detailed study of the interplay of multiple
partonic scattering and QCD radiation contributions to the
underlying event. Comparisons to the predictions of
different Monte Carlo models show a need for further model
tuning, but the standard approach is found to generally
reproduce the features of the underlying event in both types
of event selection.},
Doi = {10.1140/epjc/s10052-014-2965-5},
Key = {fds321341}
}
@article{fds331640,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandi, A and Brink,
SVD and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer,
S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold,
M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos,
K and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Guo, RS and Haas, RM and Haber, C and Hafen,
E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Herndon, M and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kirby, M and Kirk, M and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu,
YC and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman, J and Nahn, S and Nakada, H and Nakaya,
T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen,
J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pappas, SP and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom,
L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos,
F and Pukhov, O and Punzi, G and Ragan, K and Rakitine, A and Reher, D and Reichold, A and Riegler, W and Ribon, A and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Rossin, R and Safonov, A and Sakumoto,
WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
M and Spiegel, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk,
S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa, F and Vaiciulis,
T and Valls, J and III, SV and Velev, G and Vidal, R and Vilar, R and Volobouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and III,
WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh,
GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu,
Z and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Measurement of the W boson mass with the collider detector
at Fermilab},
Journal = {Physical Review D},
Volume = {64},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2001},
url = {http://dx.doi.org/10.1103/PhysRevD.64.032001},
Abstract = {We present a measurement of the W boson mass using data
collected with the CDF detector during the 1994-1995
collider run at the Fermilab Tevatron. A fit to the
transverse mass spectrum of a sample of 30115 W → ev
events recorded in an integrated luminosity of 84 pb-1 gives
a mass MW=80.473±0.065(stat) ±0.092(syst) GeV/c2. A fit to
the transverse mass spectrum of a sample of 14740 W → μν
events from 80 pb-1 gives a mass MW=80.465±0.100(stat)±0.103(syst)
GeV/c2. The dominant contributions to the systematic
uncertainties are the uncertainties in the electron energy
scale and the muon momentum scale, 0.075 GeV/c2 and 0.085
GeV/c2, respectively. The combined value for the electron
and muon channel is MW=80.470±0.089 GeV/c2. When combined
with previously published CDF measurements, we obtain
MW=80.433±0.079GeV/c2. ©2001 The American Physical
Society.},
Doi = {10.1103/PhysRevD.64.032001},
Key = {fds331640}
}
@article{fds340916,
Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
J and Culbertson, R and Dagenhart, D and D'Auria, S and Barbaro, PD and Cecco, SD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi,
C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Farrington, S and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Flores-Castillo, LR and Foster, GW and Franklin, M and Friedman, J and Furic, I and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerdes, DW and Gerstein, E and Giagu, S and Giannetti, P and Giolo, K and Giordani, M and Giromini, P and Glagolev, V and Glenzinski,
D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, SR and Halkiadakis, E and Handler, R and Happacher,
F and Hara, K and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser,
J and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hou, S and Huffman, BT and Hughes, R and Huston, J and Incandela, J and Introzzi, G and Iori, M and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jones, M and Kamon, T and Kang, J and Unel, MK and Kartal, S and Kasha, H and Kato, Y and Kennedy, RD and Kephart, R and Kilminster, B and Kim, DH and Kim, HS and Kim, MJ and Kim,
SB and Kim, SH and Kim, TH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lami, S and Lammel, S and Lancaster,
J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and LeCompte, T and Le, Y and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Mangano, M and Mariotti, M and Martin, A and Martin, M and Martin, V and Martínez, M and Mazzanti, P and McFarland, KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer,
A and Miao, T and Miller, JS and Miller, R and Miscetti, S and Mitselmakher, G and Moggi, N and Moore, R and Moulik, T and Mukherjee,
A and Mulhearn, M and Muller, T and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napora, R and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Niell, F and Nigmanov, T and Nodulman, L and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Pratt, T and Prokoshin, F and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Ratnikov,
F and Ray, H and Reichold, A and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Ryan, D and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez,
C and Sansoni, A and Santi, L and Sarkar, S and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti, A and Sill, A and Sinervo, P and Slaughter, AJ and Sliwa, K and Snider, FD and Snihur, R and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Stefanini, A and Strologas, J and Stuart, D and Sukhanov, A and Sumorok,
K and Suzuki, T and Takashima, R and Takikawa, K and Tanaka, M and Tecchio,
M and Teng, PK and Terashi, K and Tesarek, RJ and Tether, S and Thom, J and Thompson, AS and Thomson, E and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tonelli, D and Tönnesmann, M and Toyoda, H and Trischuk, W and Tseng, J and Tsybychev, D and Turini, N and Ukegawa, F and Unverhau, T and Vaiciulis, T and Varganov, A and Vataga, E and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Wagner, RG and Wagner, RL and Wagner, W and Wan, Z and Wang, C and Wang, MJ and Wang, SM and Ward, B and Waschke, S and Waters, D and Watts, T and Weber, M and III, WCW and Whitehouse, B and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
BL and Wolbers, S and Wolter, M and Worm, S and Wu, X and Würthwein, F and Yang, UK and Yao, W and Yeh, GP and Yi, K and Yoh, J and Yoshida, T and Yu, I and Yu, S and Yun, JC and Zanello, L and Zanetti, A and Zetti, F and Zucchelli,
S},
Title = {Measurement of the W boson polarization in top decay at CDF
at √s = 1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {3},
Pages = {031101-1-031101-7},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.031101},
Abstract = {The polarization of the W boson in t →Wb decay is
unambiguously predicted by the standard model of electroweak
interactions and is a powerful test of our understanding of
the tbW vertex. We measure this polarization from the
invariant mass of the b quark from t → Wb and the lepton
from W → lν whose momenta measure the W decay angle and
direction of motion, respectively. In this paper we present
a measurement of the decay rate (f V+A) of the W produced
from the decay of the top quark in the hypothesis of V + A
structure of the tWb vertex. We find no evidence for the
nonstandard V + A vertex and set a limit on fV+A < 0.80
at 95% confidence level. By combining this result with a
complementary observable in the same data, we assign a limit
on fv+A < 0.61 at 95% CL. This corresponds to a
constraint on the right-handed helicity component of the W
polarization of f+ < 0.18 at 95% CL. This limit is the
first significant direct constraint on fV+A in top decay. ©
2005 The American Physical Society.},
Doi = {10.1103/PhysRevD.71.031101},
Key = {fds340916}
}
@article{fds321288,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Measurement of the W W + W Z cross section and limits on
anomalous triple gauge couplings using final states with one
lepton, missing transverse momentum, and two jets with the
ATLAS detector at √s = 7 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {1},
Pages = {1-42},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2015)049},
Abstract = {Abstract: The production of a W boson decaying to eν or
μν in association with a W or Z boson decaying to two jets
is studied using 4.6 fb−1 of proton-proton collision data
at √s =7 TeV recorded with the ATLAS detector at the LHC.
The combined WW + WZ cross section is measured with a
significance of 3.4σ and is found to be 68±7 (stat.)±19
(syst.) pb, in agreement with the Standard Model expectation
of 61.1±2.2 pb. The distribution of the transverse momentum
of the dijet system is used to set limits on anomalous
contributions to the triple gauge coupling vertices and on
parameters of an effective-field-theory model.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP01(2015)049},
Key = {fds321288}
}
@article{fds184938,
Author = {M.C. Kruse and D. Hidas (Duke U.) and A. Abulencia et al.
(CDF collaboration)},
Title = {Measurement of the W+W - production cross section and search
for anomalous WW gamma and WWZ couplings in $p\bar{p}$
collisions at $\sqrt{s}=1.96$ TeV},
Journal = {Phys. Rev. Lett. 104, 201801},
Year = {2010},
url = {http://arXiv.org/abs/0912.4500},
Abstract = {http://arXiv.org/abs/0912.4500},
Key = {fds184938}
}
@article{fds308897,
Author = {al, FAE},
Title = {Measurement of the w-boson mass},
Journal = {Phys. Rev. Lett.},
Volume = {75},
Number = {1},
Pages = {11-16},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.75.11},
Abstract = {We present a measurement of the mass of the W boson using
data collected with the Collider Detector at Fermilab during
the 1992-93 collider run at the Fermilab Tevatron. A fit to
the transverse mass spectrum of a sample of 3268 W→μν
events recorded in an integrated luminosity of 19.7 pb-1
gives a mass MWμ=80.310±0.205(stat)±0.130(syst) GeV/c2. A
fit to 5718 W→eν events recorded in 18.2 pb-1 gives
MWe=80.490±0.145(stat) ±0.175syst GeV/c2. Combining these
results, accounting for correlated uncertainties, yields
MW=80.410±0.180 GeV/c2. © 1995 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.75.11},
Key = {fds308897}
}
@article{fds308907,
Author = {al, FAE},
Title = {Measurement of the w-boson mass},
Journal = {Phys. Rev. D},
Volume = {52},
Number = {9},
Pages = {4784-4827},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevd.52.4784},
Abstract = {© 1995 The American Physical Society This paper presents a
measurement of the mass of the W boson using data collected
with the CDF detector during the 1992-1993 collider run at
the Fermilab Tevatron. A fit to the transverse mass spectrum
of a sample of 3268 W→μν events recorded in an
integrated luminosity of 19.7 pb-1 gives MWμ=80.310±0.205
(stat)±0.130 (syst) GeV/c2. A fit to the transverse mass
spectrum of a sample of 5718 W→eν events recorded in 18.2
pb-1 gives MWe=80.490±0.145 (stat)±0.175 (syst) GeV/c2.
Combining the muon and electron results, accounting for
correlated uncertainties, yields MW=80.410±0.180
GeV/c2.},
Doi = {10.1103/physrevd.52.4784},
Key = {fds308907}
}
@article{fds321209,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of the W±Z boson pair-production
cross section in pp collisions at s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {762},
Pages = {1-22},
Publisher = {Elsevier BV},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2016.08.052},
Abstract = {The production of W±Z events in proton–proton collisions
at a centre-of-mass energy of 13 TeV is measured with the
ATLAS detector at the LHC. The collected data correspond to
an integrated luminosity of 3.2 fb−1. The W±Z candidates
are reconstructed using leptonic decays of the gauge bosons
into electrons or muons. The measured inclusive cross
section in the detector fiducial region for leptonic decay
modes is σW±Z→ℓ′νℓℓfid.=63.2±3.2(stat.)±2.6(sys.)±1.5(lumi.)
fb. In comparison, the next-to-leading-order Standard Model
prediction is 53.4−2.8+3.6 fb. The extrapolation of the
measurement from the fiducial to the total phase space
yields σW±Ztot.=50.6±2.6(stat.)±2.0(sys.)±0.9(th.)±1.2(lumi.)
pb, in agreement with a recent next-to-next-to-leading-order
calculation of 48.2−1.0+1.1 pb. The cross section as a
function of jet multiplicity is also measured, together with
the charge-dependent W+Z and W−Z cross sections and their
ratio.},
Doi = {10.1016/j.physletb.2016.08.052},
Key = {fds321209}
}
@article{fds321174,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Measurement of the WW and WZ production cross section using
final states with a charged lepton and heavy-flavor jets in
the full CDF Run II data set},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.032008},
Abstract = {We present a measurement of the total WW and WZ production
cross sections in pp collision at s=1.96 TeV, in a final
state consistent with leptonic W boson decay and jets
originating from heavy-flavor quarks from either a W or a Z
boson decay. This analysis uses the full data set collected
with the CDF II detector during Run II of the Tevatron
collider, corresponding to an integrated luminosity of 9.4
fb-1. An analysis of the dijet mass spectrum provides 3.7σ
evidence of the summed production processes of either WW or
WZ bosons with a measured total cross section of
σWW+WZ=13.7±3.9 pb. Independent measurements of the WW and
WZ production cross sections are allowed by the different
heavy-flavor decay patterns of the W and Z bosons and by the
analysis of secondary-decay vertices reconstructed within
heavy-flavor jets. The productions of WW and of WZ dibosons
are independently seen with significances of 2.9σ and
2.1σ, respectively, with total cross sections of
σWW=9.4±4.2 pb and σWZ=3.7-2.2+2.5 pb. The measurements
are consistent with standard-model predictions.},
Doi = {10.1103/PhysRevD.94.032008},
Key = {fds321174}
}
@article{fds308407,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Measurement of the WZ cross section and triple gauge
couplings in pp̄ collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.86.031104},
Abstract = {This article describes the current most precise measurement
of the WZ production cross section as well as limits on
anomalous WWZ couplings at a center-of-mass energy of 1.96
TeV in proton-antiproton collisions for the Collider
Detector at Fermilab (CDF). WZ candidates are reconstructed
from decays containing three charged leptons and missing
energy from a neutrino, where the charged leptons are either
electrons or muons. Using data collected by the CDF II
detector (7.1fb -1 of integrated luminosity), 63 candidate
events are observed with the expected background
contributing 8±1 events. The measured total cross section
σ(pp̄→WZ)=3.93-0.53+0.60(stat)-0. 46+0.59(syst)pb is in
good agreement with the standard model prediction of
3.50±0.21. The same sample is used to set limits on
anomalous WWZ couplings. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.031104},
Key = {fds308407}
}
@article{fds321337,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the Z/γ* boson transverse
momentum distribution in pp collisions at √s = 7 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {9},
Publisher = {Springer Nature},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2014)145},
Abstract = {This paper describes a measurement of the Z/γ* boson
transverse momentum spectrum using ATLAS proton-proton
collision data at a centre-of-mass energy of (Formula
presented) TeV at the LHC. The measurement is performed in
the Z/γ* → e+e− and Z/γ* → μ+μ− channels, using
data corresponding to an integrated luminosity of 4.7
fb−1. Normalized differential cross sections as a function
of the Z/γ* boson transverse momentum are measured for
transverse momenta up to 800 GeV. The measurement is
performed inclusively for Z/γ* rapidities up to 2.4, as
well as in three rapidity bins. The channel results are
combined, compared to perturbative and resummed QCD
calculations and used to constrain the parton shower
parameters of Monte Carlo generators.},
Doi = {10.1007/JHEP09(2014)145},
Key = {fds321337}
}
@article{fds321202,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram,
IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia
Bylund, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa,
A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chouridou,
S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou,
Y},
Title = {Measurement of the ZZ Production Cross Section in pp
Collisions at sqrt[s]=13 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {116},
Number = {10},
Pages = {101801},
Year = {2016},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.116.101801},
Abstract = {The ZZ production cross section in proton-proton collisions
at 13 TeV center-of-mass energy is measured using
3.2 fb^{-1} of data recorded with the ATLAS detector at
the Large Hadron Collider. The considered Z boson candidates
decay to an electron or muon pair of mass 66-116 GeV. The
cross section is measured in a fiducial phase space
reflecting the detector acceptance. It is also extrapolated
to a total phase space for Z bosons in the same mass range
and of all decay modes, giving 16.7_{-2.0}^{+2.2}(stat)+0.9/-0.7(syst)+1.0/-0.7(lumi) pb.
The results agree with standard model predictions.},
Doi = {10.1103/physrevlett.116.101801},
Key = {fds321202}
}
@article{fds308266,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Measurement of the ZZ production cross section using the
full CDF II data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.89.112001},
Abstract = {We present a measurement of the ZZ-boson pair-production
cross section in 1.96 TeV center-of-mass energy pp̄
collisions. We reconstruct final states incorporating four
charged leptons or two charged leptons and two neutrinos
from the full data set collected by the Collider Detector
experiment at the Fermilab Tevatron, corresponding to
9.7fb-1 of integrated luminosity. Combining the results
obtained from each final state, we measure a cross section
of 1.04-0.25+0.32pb, in good agreement with the standard
model prediction at next-to-leading order in the
strong-interaction coupling. © 2014 American Physical
Society.},
Doi = {10.1103/PhysRevD.89.112001},
Key = {fds308266}
}
@article{fds322005,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Measurement of the [Formula: see text] dijet cross section
in pp collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {12},
Pages = {670},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4521-y},
Abstract = {The dijet production cross section for jets containing a
b-hadron (b-jets) has been measured in proton-proton
collisions with a centre-of-mass energy of [Formula: see
text] TeV, using the ATLAS detector at the LHC. The data
used correspond to an integrated luminosity of [Formula: see
text]. The cross section is measured for events with two
identified b-jets with a transverse momentum [Formula: see
text] GeV and a minimum separation in the [Formula: see
text]-[Formula: see text] plane of [Formula: see text]. At
least one of the jets in the event is required to have
[Formula: see text] GeV. The cross section is measured
differentially as a function of dijet invariant mass, dijet
transverse momentum, boost of the dijet system, and the
rapidity difference, azimuthal angle and angular distance
between the b-jets. The results are compared to different
predictions of leading order and next-to-leading order
perturbative quantum chromodynamics matrix elements
supplemented with models for parton-showers and
hadronization.},
Doi = {10.1140/epjc/s10052-016-4521-y},
Key = {fds322005}
}
@article{fds308342,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio,
EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas,
CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
Title = {Measurement of the [Formula: see text] production cross
section in the tau + jets channel using the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {3},
Pages = {2328},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2328-7},
Abstract = {A measurement of the top quark pair production cross section
in the final state with a hadronically decaying tau lepton
and jets is presented. The analysis is based on
proton-proton collision data recorded by the ATLAS
experiment at the LHC, with a centre-of-mass energy of
7 TeV. The data sample corresponds to an integrated
luminosity of 1.67 fb<sup>-1</sup>. The cross section is
measured to be [Formula: see text] and is in agreement with
other measurements and with the Standard Model
prediction.},
Doi = {10.1140/epjc/s10052-013-2328-7},
Key = {fds308342}
}
@article{fds321368,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, MF and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
Title = {Measurement of the [Formula: see text] production
cross-section using [Formula: see text] events with
[Formula: see text]-tagged jets in [Formula: see text]
collisions at [Formula: see text] and 8 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {10},
Pages = {3109},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3109-7},
Abstract = {The inclusive top quark pair ([Formula: see text])
production cross-section [Formula: see text] has been
measured in proton-proton collisions at [Formula: see text]
and [Formula: see text] with the ATLAS experiment at the
LHC, using [Formula: see text] events with an
opposite-charge [Formula: see text] pair in the final state.
The measurement was performed with the 2011 7 TeV dataset
corresponding to an integrated luminosity of 4.6 [Formula:
see text] and the 2012 8 TeV dataset of 20.3 [Formula: see
text]. The numbers of events with exactly one and exactly
two [Formula: see text]-tagged jets were counted and used to
simultaneously determine [Formula: see text] and the
efficiency to reconstruct and [Formula: see text]-tag a jet
from a top quark decay, thereby minimising the associated
systematic uncertainties. The cross-section was measured to
be: [Formula: see text]where the four uncertainties arise
from data statistics, experimental and theoretical
systematic effects, knowledge of the integrated luminosity
and of the LHC beam energy. The results are consistent with
recent theoretical QCD calculations at next-to-next-to-leading
order. Fiducial measurements corresponding to the
experimental acceptance of the leptons are also reported,
together with the ratio of cross-sections measured at the
two centre-of-mass energies. The inclusive cross-section
results were used to determine the top quark pole mass via
the dependence of the theoretically predicted cross-section
on [Formula: see text] giving a result of [Formula: see
text][Formula: see text] GeV. By looking for an excess of
[Formula: see text] production with respect to the QCD
prediction, the results were also used to place limits on
the pair-production of supersymmetric top squarks [Formula:
see text] with masses close to the top quark mass, decaying
via [Formula: see text] to predominantly right-handed top
quarks and a light neutralino [Formula: see text], the
lightest supersymmetric particle. Top squarks with masses
between the top quark mass and 177 GeV are excluded at the
95 % confidence level.},
Doi = {10.1140/epjc/s10052-014-3109-7},
Key = {fds321368}
}
@article{fds308831,
Author = {Collboration, CDF},
Title = {Measurement of the _(W +> 1 Jet)/_ (W) Cross Section Ratio
from pp Collisions at „© s = 1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {81},
Number = {7},
Pages = {1367},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.1367},
Abstract = {The ratio of the W + ≥ 1 jet cross section to the
inclusive W cross section is measured using W±→ e±v
events from p¯p collisions at √ = 1.8 TeV. The data are
from 108pb−1 of integrated luminosity collected with the
Collider Detector at Fermilab. Measurements of the cross
section ratio for jet transverse energy thresholds(EminT)
ranging from 15 to 95 GeV are compared to theoretical
predictions using next-to-leading-order QCD calculations.
Data and theory agree well for EminT > 25 GeV, where the
predictions lie within 1 standard deviation of the measured
values. © 1998 The American Physical Society.},
Doi = {10.1103/PhysRevLett.81.1367},
Key = {fds308831}
}
@article{fds308879,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
S and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cronin-Hennessy, D and Culbertson,
R and Cunningham, JD and Daniels, T and DeJongh, F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Dunn, A and Eddy, N and Einsweiler,
K and Elias, JE and Ely, R and Jr, EE and Errede, D and Errede, S and Fan, Q and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi,
M and Freeman, J and Friedman, J and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold,
M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Guo,
RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Hardman, AD and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Hayashi, E and Heinrich, J and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes, R and Huston, J and Huth, J and Hylen, J and Ikeda, H and Incagli,
M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and Jensen, H and Joshi, U and Kadel, RW and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Keeble, L and Kelley, K and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kharadia,
B and Kim, BJ and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuwabara, T and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lu, J and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi,
E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Mitsushio, H and Miyamoto,
T and Miyashita, S and Moggi, N and Morita, Y and Mueller, J and Mukherjee,
A and Muller, T and Murat, P and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ninomiya, M and Nodulman, L and Oh, SH and Ohl, KE and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Oliveira, R and Olsen, J and Pagliarone, C and Paoletti,
R and Papadimitriou, V and Pappas, SP and Park, S and Parri, A and Patrick,
J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters,
MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Romano, J and Rosenson, L and Roser, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Scarpine, V and Schlabach, P and Schmidt, EE and Schmidt, MP and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Sganos, G and Shapiro, M and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Snider, FD and Song, T and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Strahl, K and Strait, J and Ströhmer, R and Stuart, D and Sullivan, G and Soumarokov, A and Sumorok, K and Suzuki, J and Takada, T and Takahashi, T and Takano, T and Takikawa, K and Tamura, N and Tartarelli, F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Uemura, N and Ukegawa, F and Unal, G and Brink, SVD and III, SV and Velev, G and Vidal,
R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wahl,
J and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel,
H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Wolinski, D and Wolinski,
J and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh,
GP and Yeh, P and Yin, M and Yoh, J and Yosef, C and Yoshida, T and Yovanovitch, D and Yu, I and Yu, L and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, W and Zucchelli, S},
Title = {Measurement of the Λb0 lifetime using
Λb0 → Λc+l-
ν̄},
Journal = {Physical Review Letters},
Volume = {77},
Number = {8},
Pages = {1439-1443},
Year = {1996},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.77.1439},
Abstract = {The lifetime of Λb0^ is measured using the semileptonic
decay Λb0 → Λc+l-ν-, where the Λc+ is reconstructed
through its decay Λc+ → pK- π+. The data were collected
by the CDF detector at the Tevatron Collider during
1992-1995 and correspond to an integrated luminosity of 110
pb-1 of pp̄ collisions at √s = 1.8 TeV. From a fit to the
decay length distribution of the Λc-lepton system from 197
± 25 signal events, the lifetime of Λb0 is measured to be
1.32 ± 0.15 ± 0.07 ps.},
Doi = {10.1103/physrevlett.77.1439},
Key = {fds308879}
}
@article{fds344674,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carrillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully,
JC and Cyr, D and Daronco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng,
J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube,
S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell, JL and Ginsburg,
C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute,
M and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Labarga, L and Lai, S and Lami, S and Lammel,
S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
J and Nagano, A and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prokoshin, F and Pronko, A and Proudfoot, J and Ptochos, F and Punzi, G and Pursley, J and Rademacker,
J and Rahaman, A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic,
V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti,
A},
Title = {Measurement of the Λb0 Lifetime in Λb0→J/ψΛ0 in pp̄
Collisions at s=1.96TeV},
Journal = {Physical Review Letters},
Volume = {98},
Number = {12},
Pages = {122001},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevLett.98.122001},
Abstract = {We report a measurement of the Λb0 lifetime in the
exclusive decay Λb0→J/ψΛ0 in pp̄ collisions at
s=1.96TeV using an integrated luminosity of 1.0fb-1 of data
collected by the CDF II detector at the Fermilab Tevatron.
Using fully reconstructed decays, we measure
τ(Λb0)=1.593-0.078+0.083(stat)±0.033(syst)ps. This is the
single most precise measurement of τ(Λb0) and is 3.2σ
higher than the current world average. © 2007 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.98.122001},
Key = {fds344674}
}
@article{fds321293,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
Title = {Measurement of three-jet production cross-sections in
[Formula: see text] collisions at 7 [Formula: see text]
centre-of-mass energy using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {5},
Pages = {228},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3363-3},
Abstract = {Double-differential three-jet production cross-sections are
measured in proton-proton collisions at a centre-of-mass
energy of [Formula: see text] using the ATLAS detector at
the large hadron collider. The measurements are presented as
a function of the three-jet mass [Formula: see text], in
bins of the sum of the absolute rapidity separations between
the three leading jets [Formula: see text]. Invariant masses
extending up to 5 TeV are reached for [Formula: see
text]. These measurements use a sample of data recorded
using the ATLAS detector in 2011, which corresponds to an
integrated luminosity of [Formula: see text]. Jets are
identified using the anti-[Formula: see text] algorithm with
two different jet radius parameters, [Formula: see text] and
[Formula: see text]. The dominant uncertainty in these
measurements comes from the jet energy scale.
Next-to-leading-order QCD calculations corrected to account
for non-perturbative effects are compared to the
measurements. Good agreement is found between the data and
the theoretical predictions based on most of the available
sets of parton distribution functions, over the full
kinematic range, covering almost seven orders of magnitude
in the measured cross-section values.},
Doi = {10.1140/epjc/s10052-015-3363-3},
Key = {fds321293}
}
@article{fds321149,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of top quark pair differential cross sections in
the dilepton channel in pp collisions at √s =7 and 8 TeV
with ATLAS},
Journal = {Physical Review D},
Volume = {94},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.94.092003},
Abstract = {Measurements of normalized differential cross sections of
top quark pair (tt production are presented as a function of
the mass, the transverse momentum and the rapidity of the tt
system in proton-proton collisions at center-of-mass
energies of s=7 and 8 TeV. The data set corresponds to an
integrated luminosity of 4.6 fb-1 at 7 TeV and 20.2 fb-1 at
8 TeV, recorded with the ATLAS detector at the Large Hadron
Collider. Events with top quark pair signatures are selected
in the dilepton final state, requiring exactly two charged
leptons and at least two jets with at least one of the jets
identified as likely to contain a b hadron. The measured
distributions are corrected for detector effects and
selection efficiency to cross sections at the parton level.
The differential cross sections are compared with different
Monte Carlo generators and theoretical calculations of tt
production. The results are consistent with the majority of
predictions in a wide kinematic range.},
Doi = {10.1103/PhysRevD.94.092003},
Key = {fds321149}
}
@article{fds308292,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith,
L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay,
NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach,
AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Buehrer, F and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ},
Title = {Measurement of top quark polarization in top-antitop events
from proton-proton collisions at √s=7 TeV using the
ATLAS detector.},
Journal = {Physical review letters},
Volume = {111},
Number = {23},
Pages = {232002},
Year = {2013},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.111.232002},
Abstract = {This Letter presents measurements of the polarization of the
top quark in top-antitop quark pair events, using
4.7 fb(-1) of proton-proton collision data recorded
with the ATLAS detector at the Large Hadron Collider at
√s=7 TeV. Final states containing one or two isolated
leptons (electrons or muons) and jets are considered. Two
measurements of α(ℓ)P, the product of the leptonic
spin-analyzing power and the top quark polarization, are
performed assuming that the polarization is introduced by
either a CP conserving or a maximally CP violating
production process. The measurements obtained,
α(ℓ)P(CPC)=-0.035±0.014(stat)±0.037(syst) and
α(ℓ)P(CPV)=0.020±0.016(stat)(-0.017)(+0.013)(syst), are
in good agreement with the standard model prediction of
negligible top quark polarization.},
Doi = {10.1103/physrevlett.111.232002},
Key = {fds308292}
}
@article{fds321164,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Measurement of total and differential W + W
− production cross sections in proton-proton
collisions at √s=8 TeV with the ATLAS detector and limits
on anomalous triple-gauge-boson couplings},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {9},
Publisher = {Springer Nature},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2016)029},
Abstract = {The production of W boson pairs in proton-proton collisions
at s=8 TeV is studied using data corresponding to 20.3
fb−1 of integrated luminosity collected by the ATLAS
detector during 2012 at the CERN Large Hadron Collider. The
W bosons are reconstructed using their leptonic decays into
electrons or muons and neutrinos. Events with reconstructed
jets are not included in the candidate event sample. A total
of 6636 WW candidate events are observed. Measurements are
performed in fiducial regions closely approximating the
detector acceptance. The integrated measurement is corrected
for all acceptance effects and for the W branching fractions
to leptons in order to obtain the total WW production cross
section, which is found to be 71.1 ± 1.1(stat) − 5.0+
5.7(syst) ± 1.4(lumi) pb. This agrees with the
next-to-next-to-leading-order Standard Model prediction of
63. 2− 1.4+ 1.6(scale) ± 1.2(PDF) pb. Fiducial
differential cross sections are measured as a function of
each of six kinematic variables. The distribution of the
transverse momentum of the leading lepton is used to set
limits on anomalous triple-gauge-boson couplings.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP09(2016)029},
Key = {fds321164}
}
@article{fds321217,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åesson, TPA and Akimov, AV and Alberghi,
GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and varez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of transverse energy-energy correlations in
multi-jet events in pp collisions at s=7 TeV using the ATLAS
detector and determination of the strong coupling constant
as(mZ)},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {750},
Pages = {427-447},
Publisher = {Elsevier BV},
Year = {2015},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2015.09.050},
Abstract = {High transverse momentum jets produced in pp collisions at a
centre of mass energy of 7 TeV are used to measure the
transverse energy-energy correlation function and its
associated azimuthal asymmetry. The data were recorded with
the ATLAS detector at the LHC in the year 2011 and
correspond to an integrated luminosity of 158 pb-1. The
selection criteria demand the average transverse momentum of
the two leading jets in an event to be larger than 250 GeV.
The data at detector level are well described by Monte Carlo
event generators. They are unfolded to the particle level
and compared with theoretical calculations at
next-to-leading-order accuracy. The agreement between data
and theory is good and provides a precision test of
perturbative Quantum Chromodynamics at large momentum
transfers. From this comparison, the strong coupling
constant given at the Z boson mass is determined to be
as(mZ)=0.1173±0.0010 (exp.) -0.0026+0.0065
(theo.).},
Doi = {10.1016/j.physletb.2015.09.050},
Key = {fds321217}
}
@article{fds308341,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Measurement of upsilon production in 7 TeV pp collisions at
ATLAS},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.87.052004},
Abstract = {Using 1.8 fb-1 of pp collisions at a center-of-mass energy
of 7 TeV recorded by the ATLAS detector at the Large Hadron
Collider, we present measurements of the production cross
sections of Υ(1S,2S,3S) mesons. Υ mesons are reconstructed
using the dimuon decay mode. Total production cross sections
for pT<70 GeV and in the rapidity interval |yΥ|<2.25 are
measured to be, 8.01±0.02±0.36±0.31 nb,
2.05±0.01±0.12±0.08 nb, and 0.92±0.01±0. 07±0.04 nb,
respectively, with uncertainties separated into statistical,
systematic, and luminosity measurement effects. In addition,
differential cross section times dimuon branching fractions
for Υ(1S), Υ(2S), and Υ(3S) as a function of Υ
transverse momentum pT and rapidity are presented. These
cross sections are obtained assuming unpolarized production.
If the production polarization is fully transverse or
longitudinal with no azimuthal dependence in the helicity
frame, the cross section may vary by approximately ±20%. If
a nontrivial azimuthal dependence is considered, integrated
cross sections may be significantly enhanced by a factor of
2 or more. We compare our results to several theoretical
models of Υ meson production, finding that none provide an
accurate description of our data over the full range of Υ
transverse momenta accessible with this data
set.},
Doi = {10.1103/PhysRevD.87.052004},
Key = {fds308341}
}
@article{fds314851,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of vector boson plus D∗ (2010)+ meson
production in p-p collisions at s =1.96 TeV MEASUREMENT of
VECTOR BOSON PLUS D∗ (2010)+ ... T. AALTONEN et
al.},
Journal = {Physical Review D},
Volume = {93},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {March},
ISSN = {2470-0010},
url = {http://dx.doi.org/10.1103/PhysRevD.93.052012},
Abstract = {A measurement of vector boson (V) production in conjunction
with a D∗(2010)+ meson is presented. Using a data sample
corresponding to 9.7 fb-1 of proton-antiproton collisions at
center-of-mass energy s=1.96 TeV produced by the Fermilab
Tevatron, we reconstruct V+D∗+ samples with the CDF II
detector. The D∗+ is fully reconstructed in the
D∗(2010)+→D0(→K-π+)π+ decay mode. This technique is
sensitive to the associated production of vector boson plus
charm or bottom mesons. We measure the ratio of production
cross sections σ(W+D∗)/σ(W)=[1.75±0.13(stat)±0.09(stat)]%
and σ(Z+D∗)/σ(Z)=[1.5±0.4(stat)±0.2(stat)]% and
perform a differential measurement of dσ(W+D∗)/dpT(D∗).
Event properties are utilized to determine the fraction of
V+D∗(2010)+ events originating from different production
processes. The results are in agreement with the predictions
obtained with the pythia program, limiting possible
contribution from non-standard-model physics
processes.},
Doi = {10.1103/PhysRevD.93.052012},
Key = {fds314851}
}
@article{fds308560,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D},
Title = {Measurement of W-boson helicity fractions in top-quark
decays using cos θ*},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {674},
Number = {3},
Pages = {160-167},
Publisher = {Elsevier BV},
Year = {2009},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2009.02.040},
Abstract = {Fully reconstructed t over(t, ̄) → W+ b W- over(b, ̄)
→ ℓ ν q over(q, ̄)′ b over(b, ̄) events are used to
determine the fractions of right-handed (f+) and
longitudinally polarized (f0) W bosons produced in top-quark
decays. The helicity fractions are sensitive to the
couplings and the Dirac structure of the Wtb vertex. This
Letter reports measurements of the W-boson helicity
fractions from two different methods using data
corresponding to an integrated luminosity of 1.9 fb- 1 of p
over(p, ̄) collisions at a center-of-mass energy of 1.96
TeV collected by the CDF II detector operating at the
Fermilab Tevatron. Combining the results from the two
methods, we find f0 = 0.62 ± 0.10 (stat) ± 0.05 (syst)
under the assumption that f+ = 0, and f+ = - 0.04 ± 0.04
(stat) ± 0.03 (syst) with f0 fixed to the theoretically
expected value of 0.70. Model-independent fits are also
performed and simultaneously determine f0 = 0.66 ± 0.16
(stat) ± 0.05 (syst) and f+ = - 0.03 ± 0.06 (stat) ± 0.03
(syst). All these results are consistent with standard model
expectations. © 2009 Elsevier B.V.},
Doi = {10.1016/j.physletb.2009.02.040},
Key = {fds308560}
}
@article{fds308474,
Author = {Aaltonen, and T, and others},
Title = {Measurement of W-Boson Polarization in Top-Quark Decay in
ppbar Collisions at sqrt{s}=1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {4},
Pages = {042002},
Publisher = {American Physical Society},
Year = {2010},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.042002},
Abstract = {We report measurements of the polarization of W bosons from
top-quark decays using 2.7 fb{-1} of pp collisions collected
by the CDF II detector. Assuming a top-quark mass of
175 GeV/c{2}, three measurements are performed. A
simultaneous measurement of the fraction of longitudinal
(f{0}) and right-handed (f{+}) W bosons yields the
model-independent results f{0}=0.88±0.11(stat)±0.06(syst)
and f{+}=-0.15±0.07(stat)±0.06(syst) with a correlation
coefficient of -0.59. A measurement of f{0} [f{+}]
constraining f{+} [f{0}] to its standard model value of 0.0
[0.7] yields f{0}=0.70±0.07(stat)±0.04(syst)
[f{+}=-0.01±0.02(stat)±0.05(syst)]. All these results are
consistent with standard model expectations. We achieve the
single most precise measurements of f{0} for both the
model-independent and model-dependent determinations.},
Doi = {10.1103/PhysRevLett.105.042002},
Key = {fds308474}
}
@article{fds308350,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Measurement of W-boson polarization in top-quark decay using
the full CDF Run II data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.87.031104},
Abstract = {We measure the polarization of W bosons from top-quark (t)
decays into final states with a charged lepton and jets,
tt̄→W+bW -b̄→ℓνbqq̄′b̄, using the full Run II
data set collected by the CDF II detector, corresponding to
an integrated luminosity of 8.7 fb-1. A model-independent
method simultaneously determines the fraction of
longitudinal (f0) and right-handed (f+) W bosons to yield
f0=0.726±0. 066(stat)±0.067(syst) and f+=-0.045±0.044(stat)
±0.058(syst) with a correlation coefficient of -0.69.
Additional results are presented under various standard
model assumptions. No significant discrepancies with the
standard model are observed. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.87.031104},
Key = {fds308350}
}
@article{fds308904,
Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman,
J},
Title = {Measurement of W-photon couplings in p-p-bar collisions at
sqrt s=1.8 TeV.},
Journal = {Physical review letters},
Volume = {74},
Number = {11},
Pages = {1936-1940},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.74.1936},
Abstract = {We report on a study of W + photon production in
approximately 20 pb-1 of p-p collisions at s=1.8 TeV
recorded with the Collider Detector at Fermilab. Our results
are in good agreement with standard model expectations and
are used to obtain limits on anomalous CP-conserving WW
couplings of -2.3<<2.2 for =0 and -0.7<<0.7 for =0 at 95%
C.L. We obtain the same limits for CP-violating couplings.
These results provide limits on the higher-order
electromagnetic moments of the W boson of 0.8<gW<3.1 for
qWe=1 and -0.6<qWe<2.7 for gW=2 at 95% C.L. © 1995 The
American Physical Society.},
Doi = {10.1103/physrevlett.74.1936},
Key = {fds308904}
}
@article{fds308714,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery,
M},
Title = {Measurement of Wγ and Zγ production
in pp̄ collisions at √s = 1.96 TeV},
Journal = {Physical Review Letters},
Volume = {94},
Number = {4},
Year = {2005},
Month = {February},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.94.041803},
Abstract = {The standard model predictions for Wγ and Z γ production
are tested using an integrated luminosity of 200 pb-1 of
pp̄ collision data collected at the Collider Detector at
Fermilab. The cross sections are measured by selecting
leptonic decays of the W and Z bosons, and photons with
transverse energy ET > 7 GeV that are well separated from
leptons. The production cross sections and kinematic
distributions for the Wγ and Zγ data are compared to SM
predictions. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.94.041803},
Key = {fds308714}
}
@article{fds322487,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and AlconadaVerzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of W+W-production in
association with one jet in proton-proton collisions at √s
= 8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {763},
Pages = {114-133},
Publisher = {Elsevier BV},
Year = {2016},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2016.10.014},
Abstract = {The production of Wboson pairs in association with one jet
in pp collisions at √s = 8 TeV is studied using data
corresponding to an integrated luminosity of 20.3
fb-1collected by the ATLAS detector during 2012 at the CERN
Large Hadron Collider. The cross section is measured in a
fiducial phase-space region defined by the presence of
exactly one electron and one muon, missing transverse
momentum and exactly one jet with a transverse momentum
above 25 GeV and a pseudorapidity of |η| <4.5. The leptons
are required to have opposite electric charge and to pass
transverse momentum and pseudorapidity requirements. The
fiducial cross section is found to be σWWfid,1-jet= 136 ±
6 (stat)± 14 (syst)± 3 (lumi) fb. In combination with a
previous measurement restricted to leptonic final states
with no associated jets, the fiducial cross section of WW
production with zero or one jet is measured to be
σWWfid,≤1-jet= 511 ±9 (stat)±26 (syst)±10 (lumi)fb.
The ratio of fiducial cross sections in final states with
one and zero jets is determined to be 0.36 ±0.05. Finally,
a total cross section extrapolated from the fiducial
measurement of WW production with zero or one associated jet
is reported. The measurements are compared to theoretical
predictions and found in good agreement.},
Doi = {10.1016/j.physletb.2016.10.014},
Key = {fds322487}
}
@article{fds321173,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Measurement of W± and Z-boson production cross
sections in pp collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {759},
Pages = {601-621},
Publisher = {Elsevier BV},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2016.06.023},
Abstract = {Measurements of the W±→ℓ±ν and Z→ℓ+ℓ−
production cross sections (where ℓ±=e±,μ±) in
proton–proton collisions at s=13 TeV are presented using
data recorded by the ATLAS experiment at the Large Hadron
Collider, corresponding to a total integrated luminosity of
81 pb−1. The total inclusive W±-boson production cross
sections times the single-lepton-flavour branching ratios
are σW+tot=11.83±0.02 (stat)±0.32 (sys)±0.25 (lumi) nb
and σW−tot=8.79±0.02 (stat)±0.24 (sys)±0.18 (lumi) nb
for W+ and W−, respectively. The total inclusive Z-boson
production cross section times leptonic branching ratio,
within the invariant mass window 66<mℓℓ<116 GeV, is
σZtot=1.981±0.007 (stat)±0.038 (sys)±0.042 (lumi) nb.
The W+, W−, and Z-boson production cross sections and
cross-section ratios within a fiducial region defined by the
detector acceptance are also measured. The cross-section
ratios benefit from significant cancellation of experimental
uncertainties, resulting in σW+fid/σW−fid=1.295±0.003
(stat)±0.010 (sys) and σW±fid/σZfid=10.31±0.04
(stat)±0.20 (sys). Theoretical predictions, based on
calculations accurate to next-to-next-to-leading order for
quantum chromodynamics and to next-to-leading order for
electroweak processes and which employ different parton
distribution function sets, are compared to these
measurements.},
Doi = {10.1016/j.physletb.2016.06.023},
Key = {fds321173}
}
@article{fds308810,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbara, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla,
G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir,
S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch,
H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel,
O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti,
G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton,
R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Hohlmann,
M and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman,
BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins,
D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch,
L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo,
K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald,
W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone,
S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang,
CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli,
S},
Title = {Measurement of Z0 and Drell-Yan production cross
sections using dimuons in p̄p collisions at
√s=1.8TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {59},
Number = {5},
Pages = {1-15},
Year = {1999},
Abstract = {We present a measurement of Z0 boson and Drell-Yan
production cross sections in p̄p collisions at √s =1.8TeV
using a sample of 107 pb-1 accumulated by the Collider
Detector at Fermilab. The Drell-Yan cross section is
measured in the mass range of Mμμ>40GeV/c2. We compare
the measurements with the predictions of quantum
chromodynamics in both leading order and next-to-leading
order, incorporating the recent parton distribution
functions. The measurements are consistent with the standard
model expectations. ©1999 The American Physical
Society.},
Key = {fds308810}
}
@article{fds308393,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of ZZ production in leptonic final states at
sqrt[s] of 1.96 TeV at CDF.},
Journal = {Physical review letters},
Volume = {108},
Number = {10},
Pages = {101801},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.108.101801},
Abstract = {In this Letter, we present a precise measurement of the
total ZZ production cross section in pp collisions at
sqrt[s]=1.96 TeV, using data collected with the CDF II
detector corresponding to an integrated luminosity of
approximately 6 fb(-1). The result is obtained by
combining separate measurements in the four-charged
(ℓℓℓ' ℓ') and two-charged-lepton and
two-neutral-lepton (ℓℓνν) decay modes of the Z boson
pair. The combined measured cross section for pp → ZZ is
1.64(-0.38)(+0.44) pb. This is the most precise
measurement of the ZZ production cross section in 1.96 TeV
pp collisions to date.},
Doi = {10.1103/physrevlett.108.101801},
Key = {fds308393}
}
@article{fds308344,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Measurement of ZZ production in pp collisions at √ = 7 TeV
and limits on anomalous ZZZ and ZZγ couplings with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {3},
Publisher = {Springer Nature},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2013)128},
Abstract = {A measurement of the ZZ production cross section in
proton-proton collisions at √ = 7 TeV using data recorded
by the ATLAS experiment at the Large Hadron Collider is
presented. In a data sample corresponding to an integrated
luminosity of 4.6 fb-1 collected in 2011, events are
selected that are consistent either with two Z bosons
decaying to electrons or muons or with one Z boson decaying
to electrons or muons and a second Z boson decaying to
neutrinos. The ZZ → ℓ + ℓ - ℓ ′+ ℓ ′- and ZZ
→ ℓ + ℓ - ℓv̄v cross sections are measured in
restricted phase-space regions. These results are then used
to derive the total cross section for ZZ events produced
with both Z bosons in the mass range 66 to 116 GeV, σZZtot
= 6.7 ± 0.7 (stat.) -0.3+0.4 (stat.) ± 0.3 (lumi.) pb,
which is consistent with the Standard Model prediction of
5.89-0.18+0.22 pb calculated at next-to-leading order in
QCD. The normalized differential cross sections in bins of
various kinematic variables are presented. Finally, the
differential event yield as a function of the transverse
momentum of the leading Z boson is used to set limits on
anomalous neutral triple gauge boson couplings in ZZ
production. © 2013 Cern for the benefit of the ATLAS
collaboration.},
Doi = {10.1007/JHEP03(2013)128},
Key = {fds308344}
}
@article{fds375948,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport, PP and Aloisio,
A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev,
V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Measurement of Zγγ production in pp collisions at √s=13
TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11579-8},
Abstract = {Cross-sections for the production of a Z boson in
association with two photons are measured in proton–proton
collisions at a centre-of-mass energy of 13 TeV. The data
used correspond to an integrated luminosity of 139 fb - 1
recorded by the ATLAS experiment during Run 2 of the LHC.
The measurements use the electron and muon decay channels of
the Z boson, and a fiducial phase-space region where the
photons are not radiated from the leptons. The integrated
Z(→ ℓℓ) γγ cross-section is measured with a
precision of 12% and differential cross-sections are
measured as a function of six kinematic variables of the
Zγγ system. The data are compared with predictions from MC
event generators which are accurate to up to next-to-leading
order in QCD. The cross-section measurements are used to set
limits on the coupling strengths of dimension-8 operators in
the framework of an effective field theory.},
Doi = {10.1140/epjc/s10052-023-11579-8},
Key = {fds375948}
}
@article{fds308778,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den
Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer,
E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, M and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell’Agnello, S and Dell’Orso,
M},
Title = {Measurement of [Formula Presented] for high mass Drell-Yan
[Formula Presented] pairs from [Formula Presented]
collisions at [Formula Presented] TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {63},
Number = {1},
Pages = {111011-111016},
Year = {2001},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.63.011101},
Abstract = {We report on the first measurement of the rapidity
distribution [Formula Presented] over nearly the entire
kinematic region of rapidity for [Formula Presented] pairs
in both the Z-boson region of [Formula Presented] and in the
high mass region of [Formula Presented] The data sample
consists of 108 [Formula Presented] of [Formula Presented]
collisions at [Formula Presented] TeV taken by the Collider
Detector at Fermilab during 1992–1995. The total cross
section in the Z-boson region is measured to be [Formula
Presented] pb. The measured total cross section and [Formula
Presented] are compared with quantum chromodynamics
calculations in leading and higher orders. © 2000 The
American Physical Society.},
Doi = {10.1103/PhysRevD.63.011101},
Key = {fds308778}
}
@article{fds314152,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Antos, J and Apollinari, G and Arisawa,
T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge,
JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker,
C and Bloom, K and Blumenfeld, B and Blusk, BS and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and van den Brink, S and Bromberg, C and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto,
G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Cobal, M and Cocca, E and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Guimaraes da Costa and J and Costanzo, D and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F},
Title = {Measurement of [formula presented] from [formula presented]
with the CDF detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {61},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.61.072005},
Abstract = {This paper reports an updated measurement of the standard
model (Formula presented) violation parameter (Formula
presented) using the CDF Detector at Fermilab. The entire
run I data sample of (Formula presented) of
proton-antiproton collisions at (Formula presented) is used
to identify a signal sample of (Formula presented) events,
where (Formula presented) and (Formula presented) The flavor
of the neutral B meson is identified at the time of
production by combining information from three tagging
algorithms: a same-side tag, a jet-charge tag, and a
soft-lepton tag. A maximum likelihood fitting method is used
to determine (Formula presented) This value of (Formula
presented) is consistent with the standard model prediction,
based upon existing measurements, of a large positive
(Formula presented)-violating asymmetry in this decay mode.
© 2000 The American Physical Society.},
Doi = {10.1103/PhysRevD.61.072005},
Key = {fds314152}
}
@article{fds308853,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg,
C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane,
D and Cronin-Hennessy, D and Culbertson, R and Daniels, T and DeJongh,
F and Delchamps, S and Dell’Agnello, S and Dell’Orso, M and Demina,
R and Demortier, L},
Title = {Measurement of [Formula presented] production correlations,
[Formula presented] mixing, and a limit on [Formula
presented] in [Formula presented] collisions at [Formula
presented] TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {55},
Number = {5},
Pages = {2546-2558},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.55.2546},
Abstract = {We present measurements of correlated [Formula presented]
cross sections, [Formula presented] correlations, the
average [Formula presented] mixing parameter [Formula
presented], and a limit on the CP-violating parameter
[Formula presented] For these measurements, we use muon
pairs from [Formula presented] double semileptonic decays.
The data used in this analysis were taken with the Collider
Detector at Fermilab and represent an integrated luminosity
of [Formula presented] pb[Formula presented]. The results
concerning [Formula presented] production correlations are
compared to predictions of next-to-leading order QCD
computations. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevD.55.2546},
Key = {fds308853}
}
@article{fds308765,
Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera,
S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan,
AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Colijn, AP and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R},
Title = {Measurement of [Formula Presented]-meson lifetimes using
fully reconstructed [Formula Presented] decays produced in
[Formula Presented] collisions at [Formula
Presented]},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {65},
Number = {9},
Pages = {7},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.65.092009},
Abstract = {We present an improved measurement of b-meson lifetimes
using fully reconstructed B-decays produced in (Formula
presented) collisions at (Formula presented) using (Formula
presented) of data collected at the Collider Detector at
Fermilab. We obtain (Formula presented) (Formula presented)
and for the lifetime ratio (Formula presented). © 2002 The
American Physical Society.},
Doi = {10.1103/PhysRevD.65.092009},
Key = {fds308765}
}
@article{fds308644,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
MA},
Title = {Measurement of σ(pp̄→Z)•B(Z→ττ) in pp̄ collisions
at s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {75},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2007},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.75.092004},
Abstract = {We present a measurement of the inclusive production cross
section for Z bosons decaying to tau leptons in pp̄
collisions at s=1.96TeV. We use a channel with one
hadronically-decaying and one electronically-decaying tau.
This measurement is based on 350pb-1 of CDF Run II data.
Using a sample of 504 opposite sign eτ events with a total
expected background of 190 events, we obtain
σ(pp̄→4Z)•B(Z→ττ)=264±23(stat)
±14(syst)±15(lumi)pb, in agreement with the
next-to-next-to- leading order QCD prediction. This is the
first CDF cross section measurement using
hadronically-decaying taus in Run II. © 2007 The American
Physical Society.},
Doi = {10.1103/PhysRevD.75.092004},
Key = {fds308644}
}
@article{fds308886,
Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cen, Y and Cervelli, F and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cunningham, JD and Daniels, T and DeJongh, F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dickson, M and Dittmann,
JR and Donati, S and Drucker, RB and Dunn, A and Einsweiler, K and Elias,
JE and Ely, R and Jr, EE and Eno, S and Errede, D and Errede, S and Fan, Q and Farhat, B and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman, J and Frisch, H and Fry, A and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro, M and Garfinkel, AF and Geer, S and Gerdes, DW and Giannetti,
P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold, M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Grewal, A and Groer, L and Grosso-Pilcher, C and Haber,
C and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Heinrich, J and Cronin-Hennessy, D and Hollebeek, R and Holloway, L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes,
R and Hurst, P and Huston, J and Huth, J and Hylen, J and Incagli, M and Incandela, J and Iso, H and Jensen, H and Jessop, CP and Joshi, U and Kadel, RW and Kajfasz, E and Kamon, T and Kaneko, T and Kardelis, DA and Kasha, H and Kato, Y and Keeble, L and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Loomis, C and Long, O and Loreti, M and Low, EH and Lu, J and Lucchesi, D and Luchini,
CB and Lukens, P and Lys, J and Maas, P and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Michail, G and Mikamo, S and Miller, M and Miller, R and Mimashi, T and Miscetti, S and Mishina, M and Mitsushio, H and Miyashita, S and Morita, Y and Moulding,
S and Mueller, J and Mukherjee, A and Muller, T and Musgrave, P and Nakae,
LF and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Nodulman, L and Ogawa, S and Oh, SH and Ohl, KE and Oishi, R and Okusawa,
T and Pagliarone, C and Paoletti, R and Papadimitriou, V and Park, S and Patrick, J and Pauletta, G and Paulini, M and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Plunkett, R and Pondrom, L and Produit, N and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Rimondi, F and Ristori, L and Roach-Bellino, M and Robertson, WJ and Rodrigo, T and Romano, J and Rosenson, L and Sakumoto,
WK and Saltzberg, D and Sansoni, A and Scarpine, V and Schindler, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schneider, O and Sciacca, GF and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Sganos, G and Sgolacchia, A and Shapiro, M and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Smith, DA and Snider, FD and Song, L and Song, T and Spalding, J and Spiegel, L and Sphicas, P and Spies, A and Stanco, L and Steele, J and Stefanini, A and Strahl, K and Strait, J and Stuart, D and Sullivan, G and Sumorok, K and Jr, RLS and Takahashi, T and Takikawa, K and Tartarelli, F and Taylor,
W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, J and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov, A and Tkaczyk,
S and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Tseng, J and Turcotte, M and Turini, N and Uemura, N and Ukegawa, F and Unal, G and Brink, SCVD and III, SV and Vidal, R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wainer, N and Walker, RC and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, G and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and III, WCW and Westhusing, T and Wicklund, AB and Wicklund,
E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Wolinski, J and Wu, DY and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef,
C and Yoshida, T and Yovanovitch, D and Yu, I and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, S and Zhang, W and Zucchelli,
S},
Title = {Measurement of σB(W→ev) and σB(Z0→e+e-)
in pp̄ collisions at √s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {76},
Number = {17},
Pages = {3070-3075},
Year = {1996},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.76.3070},
Abstract = {We present a measurement of σB(W → ev) and σB(Z0 →
e+e-) in proton-antiproton collisions at √s = 1.8 TeV
using a significantly improved understanding of the
integrated luminosity. The data represent an integrated
luminosity of 19.7 pb-1 from the 1992-1993 run with the
Collider Detector at Fermilab. We find σB(W → ev) = 2.49
± 0.12 nb and σB(Z0 ?→ e+e- = 0.231 ± 0.012
nb.},
Doi = {10.1103/physrevlett.76.3070},
Key = {fds308886}
}
@article{fds344672,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully,
JC and Cyr, D and Daronco, S and Datta, M and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher,
A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube,
S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell, JL and Ginsburg,
C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic, V and Renton,
P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P},
Title = {Measurement of σχc2B(χc2→J/ψγ)/ σχc1B(χc1→J/ψγ)
in pp̄ Collisions at s=1.96TeV},
Journal = {Physical Review Letters},
Volume = {98},
Number = {23},
Pages = {232001},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevLett.98.232001},
Abstract = {We measure the ratio of cross section times branching
fraction, Rp=σχc2B(χc2→J/ψγ)/σχc1B(χc1→J/ ψγ),
in 1.1fb-1 of pp̄ collisions at s=1.96TeV. This measurement
covers the kinematic range pT(J/ψ)>4.0GeV/c,
η(J/ψ)<1.0, and pT(γ)>1.0GeV/c. For events due to
prompt processes, we find Rp=0.395±0.016(stat)±0.015(syst).
This result represents a significant improvement in
precision over previous measurements of prompt χc1,2 hadro
production. © 2007 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.98.232001},
Key = {fds344672}
}
@article{fds325312,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Da Barreiro Guimarães Costa and J and Bartoldus,
R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes,
GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and De Bruckman Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burghgrave,
B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey,
P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Cherkaoui Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M},
Title = {Measurement of χc1 and ψχc2 production with √s = 7 TeV
pp collisions at ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {7},
Pages = {1-51},
Publisher = {Springer Verlag},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2014)154},
Abstract = {The prompt and non-prompt production cross-sections for the
χc1 and χc2 charmonium states are measured in pp
collisions at √s = 7TeV with the ATLAS detector at the LHC
using 4.5 fb−1 of integrated luminosity. The χc states
are reconstructed through the radiative decay χc → J/ψγ
(with J/ψ → μ+μ−) where photons are reconstructed
from γ → e+e− conversions. The production rate of the
χc2 state relative to the χc1 state is measured for prompt
and non-prompt χc as a function of J/ψ transverse
momentum. The prompt χc cross-sections are combined with
existing measurements of prompt J/ψ production to derive
the fraction of prompt J/ψ produced in feed-down from χc
decays. The fractions of χc1 and χc2 produced in b-hadron
decays are also measured.},
Doi = {10.1007/JHEP07(2014)154},
Key = {fds325312}
}
@article{fds308759,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Measurement with the ATLAS detector of multi-particle
azimuthal correlations in p + Pb collisions at
√sNN= 5.02 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {725},
Number = {1-3},
Pages = {60-78},
Publisher = {Elsevier BV},
Year = {2013},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2013.06.057},
Abstract = {In order to study further the long-range correlations
("ridge") observed recently in p + Pb collisions at √sNN=
5.02 TeV, the second-order azimuthal anisotropy parameter of
charged particles, v2, has been measured with the cumulant
method using the ATLAS detector at the LHC. In a data sample
corresponding to an integrated luminosity of approximately 1
μb-1, the parameter v2has been obtained using two- and
four-particle cumulants over the pseudorapidity range
|η|<2.5. The results are presented as a function of
transverse momentum and the event activity, defined in terms
of the transverse energy summed over 3.1 < η <4.9 in the
direction of the Pb beam. They show features characteristic
of collective anisotropic flow, similar to that observed in
Pb + Pb collisions. A comparison is made to results obtained
using two-particle correlation methods, and to predictions
from hydrodynamic models of p +Pb collisions. Despite the
small transverse spatial extent of the p + Pb collision
system, the large magnitude of v2and its similarity to
hydrodynamic predictions provide additional evidence for the
importance of final-state effects in p + Pb reactions. ©
2013 CERN. Published by Elsevier B.V.},
Doi = {10.1016/j.physletb.2013.06.057},
Key = {fds308759}
}
@article{fds308727,
Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
J and Culbertson, R and Dagenhart, D and D'Auria, S and Barbaro, PD and Cecco, SD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi,
C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Farrington, S and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Flores-Castillo, LR and Foster, GW and Franklin, M and Friedman, J and Furic, I and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerdes, DW and Gerstein, E and Giagu, S and Giannetti, P and Giolo, K and Giordani, M and Giromini, P and Glagolev, V and Glenzinski,
D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, SR and Halkiadakis, E and Handler, R and Happacher,
F and Hara, K and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser,
J and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hou, S and Huffman, BT and Hughes, R and Huston, J and Issever, C and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jones, M and Kamon, T and Kang, J and Unel, MK and Kartal, S and Kasha, H and Kato, Y and Kennedy, RD and Kephart, R and Kilminster, B and Kim, DH and Kim, HS and Kim, MJ and Kim,
SB and Kim, SH and Kim, TH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lami, S and Lammel, S and Lancaster,
J and Lannon, K and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Le, Y and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Liu, T and Litvintsev, DO and Lockyer, NS and Loginov, A and Loreti, M and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Manca, G and Mariotti, M and Martin, M and Martin, A and Martin, V and Martínez, M and Mazzanti, P and McFarland, KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer,
A and Miao, T and Miller, R and Miller, JS and Miscetti, S and Mitselmakher, G and Moggi, N and Moore, R and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napora, R and Niell, F and Nelson, C and Nelson,
T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nigmanov, T and Nodulman, L and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Pompo, A and Pondrom, L and Pope, G and Pratt, T and Prokoshin, F and Proudfoot, J and Ptohos, F and Poukhov, O and Punzi, G and Rademacker, J and Rakitine, A and Ratnikov,
F and Ray, H and Reichold, A and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Ryan, D and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez,
C and Sansoni, A and Santi, L and Sarkar, S and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti, A and Sill, A and Sinervo, P and Slaughter, AJ and Sliwa, K and Snider, FD and Snihur, R and Spezziga, M and Spinella, F and Spiropulu, M and Spiegel, L and Stefanini, A and Strologas, J and Stuart, D and Sukhanov, A and Sumorok,
K and Suzuki, T and Takashima, R and Takikawa, K and Tanaka, M and Tecchio,
M and Tesarek, RJ and Teng, PK and Terashi, K and Tether, S and Thom, J and Thompson, AS and Thomson, E and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tonelli, D and Tönnesmann, M and Toyoda, H and Trischuk, W and Tseng, J and Tsybychev, D and Turini, N and Ukegawa, F and Unverhau, T and Vaiciulis, T and Varganov, A and Vataga, E and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Wagner, RG and Wagner, RL and Wagner, W and Wan, Z and Wang, C and Wang, MJ and Wang, SM and Ward, B and Waschke, S and Waters, D and Watts, T and Weber, M and III, WCW and Whitehouse, B and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
BL and Wolbers, S and Wolter, M and Worm, S and Wu, X and Würthwein, F and Yang, UK and Yao, W and Yeh, GP and Yi, K and Yoh, J and Yoshida, T and Yu, I and Yu, S and Yun, JC and Zanello, L and Zanetti, A and Zetti, F and Zucchelli,
S},
Title = {Measurements of bottom-antibottom azimuthal production
correlations in proton-antiproton collisions at
s=1.8TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {9},
Pages = {1-39},
Year = {2005},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.71.092001},
Abstract = {We have measured the azimuthal angular correlation of bb̄
production, using 86.5pb-1 of data collected by Collider
Detector at Fermilab (CDF) in pp̄ collisions at s=1.8TeV
during 1994-1995. In high-energy pp̄ collisions, such as at
the Tevatron, bb̄ production can be schematically
categorized into three mechanisms. The leading-order (LO)
process is "flavor creation," where both b and b̄ quarks
substantially participate in the hard scattering and result
in a distinct back-to-back signal in final state. The
"flavor excitation" and the "gluon splitting" processes,
which appear at next-leading-order (NLO), are known to make
a comparable contribution to total bb̄ cross section, while
providing very different opening angle distributions from
the LO process. An azimuthal opening angle between bottom
and antibottom, Δ, has been used for the correlation
measurement to probe the interaction creating bb̄ pairs.
The Δ distribution has been obtained from two different
methods. One method measures the Δ between bottom hadrons
using events with two reconstructed secondary vertex tags.
The other method uses bb̄→(J/ ψX)(X′) events, where
the charged lepton () is an electron (e) or a muon (μ), to
measure Δ between bottom quarks. The bb̄ purity is
determined as a function of Δ by fitting the decay length
of the J/ψ and the impact parameter of the. Both methods
quantify the contribution from higher-order production
mechanisms by the fraction of the bb̄ pairs produced in the
same azimuthal hemisphere, ftoward. The measured ftoward
values are consistent with both parton shower Monte Carlo
and NLO QCD predictions. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevD.71.092001},
Key = {fds308727}
}
@article{fds308464,
Author = {Aaltonen, and T, and others},
Title = {Measurements of branching fraction ratios and
$CP$-asymmetries in suppressed ${B}^{-}\rightarrow
D(\rightarrow{K}^{+}{\pi}^{-}){K}^{-}$ and
${B}^{-}\rightarrow D(\rightarrow{K}^{+} \pi^{-}){\pi}^{-}$
decays},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {9},
Pages = {091504},
Publisher = {American Physical Society},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.84.091504},
Abstract = {We report the first reconstruction in hadron collisions of
the suppressed decays B-→D(→K+π-)K- and
B-→D(→K+π-)π-, sensitive to the Cabibbo-Kobayashi-Maskawa
phase γ, using data from 7 fb-1 of integrated
luminosity collected by the CDF II detector at the Tevatron
collider. We reconstruct a signal for the B-→D(→K+π-)K-
suppressed mode with a significance of 3.2 standard
deviations, and measure the ratios of the suppressed to
favored branching fractions R(K)=[22.0$\pm$8.6(stat)$\pm$2.6(syst)]×10-3,
R+(K)=[42.6$\pm$13.7(stat)$\pm$2.8(syst)]×10-3,
R-(K)=[3.8$\pm$10.3(stat)$\pm$2.7(syst)]×10-3 as well as
the direct CP-violating asymmetry A(K)=-0.82$\pm$0.44(stat)$\pm$0.09(syst)
of this mode. Corresponding quantities for
B-→D(→K+π-)π- decay are also reported.},
Doi = {10.1103/PhysRevD.84.091504},
Key = {fds308464}
}
@article{fds308500,
Author = {Aaltonen, and T, and others},
Title = {Measurements of branching fraction ratios and CP asymmetries
in $B^\pm \to D_{CP} K^\pm$ decays in hadron
collisions},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {3},
Pages = {031105},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.031105},
Abstract = {http://arxiv.org/abs/0911.0425},
Doi = {10.1103/PhysRevD.81.031105},
Key = {fds308500}
}
@article{fds375910,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez, AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Dos Santos and SPA and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Measurements of differential cross sections of Higgs boson
production through gluon fusion in the H→
WW*→ eνμν final state at √s=13 TeV with
the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {9},
Year = {2023},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11873-5},
Abstract = {Higgs boson production via gluon–gluon fusion is measured
in the WW*? e?µ? decay channel. The dataset utilized
corresponds to an integrated luminosity of 139 fb - 1
collected by the ATLAS detector from s=13 TeV
proton–proton collisions delivered by the Large Hadron
Collider between 2015 and 2018. Differential cross sections
are measured in a fiducial phase space restricted to the
production of at most one additional jet. The results are
consistent with Standard Model expectations, derived using
different Monte Carlo generators.},
Doi = {10.1140/epjc/s10052-023-11873-5},
Key = {fds375910}
}
@article{fds365384,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Measurements of differential cross-sections in four-lepton
events in 13 TeV proton-proton collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2021)005},
Abstract = {Measurements of four-lepton differential and integrated
fiducial cross-sections in events with two same-flavour,
opposite-charge electron or muon pairs are presented. The
data correspond to 139 fb−1 of s = 13 TeV proton-proton
collisions, collected by the ATLAS detector during Run 2 of
the Large Hadron Collider (2015–2018). The final state has
contributions from a number of interesting Standard Model
processes that dominate in different four-lepton invariant
mass regions, including single Z boson production, Higgs
boson production and on-shell ZZ production, with a complex
mix of interference terms, and possible contributions from
physics beyond the Standard Model. The differential
cross-sections include the four-lepton invariant mass
inclusively, in slices of other kinematic variables, and in
different lepton flavour categories. Also measured are
dilepton invariant masses, transverse momenta, and angular
correlation variables, in four regions of four-lepton
invariant mass, each dominated by different processes. The
measurements are corrected for detector effects and are
compared with state-of-the-art Standard Model calculations,
which are found to be consistent with the data. The Z →
4ℓ branching fraction is extracted, giving a value of
(4.41 ± 0.30) × 10−6. Constraints on effective field
theory parameters and a model based on a spontaneously
broken B − L gauge symmetry are also evaluated. Further
reinterpretations can be performed with the provided
information. [Figure not available: see fulltext.]},
Doi = {10.1007/JHEP07(2021)005},
Key = {fds365384}
}
@article{fds308438,
Author = {Aaltonen, and T, and al, E},
Title = {Measurements of Direct ${CP}$ Violating Asymmetries in
Charmless Decays of Strange Bottom Mesons and Bottom
Baryons},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {18},
Pages = {181802},
Publisher = {American Physical Society},
Year = {2011},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.181802},
Abstract = {We report measurements of direct CP-violating asymmetries in
charmless decays of neutral bottom hadrons to pairs of
charged hadrons with the upgraded Collider Detector at the
Fermilab Tevatron. Using a data sample corresponding to 1
fb(-1) of integrated luminosity, we obtain the first
measurements of direct CP violation in bottom strange
mesons, A(CP)(B(s)(0)→K(-)π(+))=+0.39±0.15(stat)±0.08(syst),
and bottom baryons, A(CP)(Λ(b)(0)→pπ(-))=+0.03±0.17(stat)±0.05(syst)
and A(CP)(Λ(b)(0)→pK(-))=+0.37±0.17(stat)±0.03(syst).
In addition, we measure CP violation in B(0)→K(+)π(-)
decays with 3.5σ significance, A(CP)(B(0)→K(+)π(-))=-0.086±0.023(stat)±0.009(syst),
in agreement with the current world average. Measurements of
branching fractions of B(s)(0)→K(+)K(-) and
B(0)→π(+)π(-) decays are also updated.},
Doi = {10.1103/PhysRevLett.106.181802},
Key = {fds308438}
}
@article{fds314178,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurements of fiducial and differential cross sections for
Higgs boson production in the diphoton decay channel at √s
= 8 TeV with ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {9},
Pages = {1-60},
Year = {2014},
Month = {September},
ISSN = {1126-6708},
url = {http://dx.doi.org/10.1007/JHEP09(2014)112},
Abstract = {Measurements of fiducial and differential cross sections are
presented for Higgs boson production in proton-proton
collisions at a centre-of-mass energy of √s = 8TeV. The
analysis is performed in the H → γγ decay channel using
20.3 fb−1 of data recorded by the ATLAS experiment at the
CERN Large Hadron Collider. The signal is extracted using a
fit to the diphoton invariant mass spectrum assuming that
the width of the resonance is much smaller than the
experimental resolution. The signal yields are corrected for
the effects of detector inefficiency and resolution. The pp
→ H → γγ fiducial cross section is measured to be 43.2
±9.4 (stat.) +3.2−2.9 (syst.) ±1.2 (lumi) fb for a Higgs
boson of mass 125.4 GeV decaying to two isolated photons
that have transverse momentum greater than 35% and 25% of
the diphoton invariant mass and each with absolute
pseudorapidity less than 2.37. Four additional fiducial
cross sections and two cross-section limits are presented in
phase space regions that test the theoretical modelling of
different Higgs boson production mechanisms, or are
sensitive to physics beyond the Standard Model. Differential
cross sections are also presented, as a function of
variables related to the diphoton kinematics and the jet
activity produced in the Higgs boson events. The observed
spectra are statistically limited but broadly in line with
the theoretical expectations.},
Doi = {10.1007/JHEP09(2014)112},
Key = {fds314178}
}
@article{fds308265,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JC and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC},
Title = {Measurements of four-lepton production at the Z resonance in
pp collisions at sqrt[s] = 7 and 8 TeV with
ATLAS.},
Journal = {Physical review letters},
Volume = {112},
Number = {23},
Pages = {231806},
Year = {2014},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.112.231806},
Abstract = {Measurements of four-lepton (4ℓ, ℓ=e,μ) production
cross sections at the Z resonance in pp collisions at the
LHC with the ATLAS detector are presented. For dilepton and
four-lepton invariant mass regions m(ℓ+ℓ(-)) > 5 GeV and
80<m(4ℓ) < 100 GeV, the measured cross sections are 76 ±
18(stat) ± 4(syst) ± 1.4(lumi) fb and 107 ± 9(stat) ±
4(syst) ± 3.0(lumi) fb at sqrt[s] = 7 and 8 TeV,
respectively. By subtracting the nonresonant 4ℓ production
contributions and normalizing with Z → μ(+)μ(-) events,
the branching fraction for the Z boson decay to 4ℓ is
determined to be (3.20 ± 0.25(stat) ± 0.13(syst)) ×
10(-6), consistent with the standard model
prediction.},
Doi = {10.1103/physrevlett.112.231806},
Key = {fds308265}
}
@article{fds308317,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and AbdelKhalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
M},
Title = {Measurements of Higgs boson production and couplings in
diboson final states with the ATLAS detector at the
LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {726},
Number = {1-3},
Pages = {88-119},
Publisher = {Elsevier BV},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2013.08.010},
Abstract = {Measurements are presented of production properties and
couplings of the recently discovered Higgs boson using the
decays into boson pairs, H→γγ, H→ZZ*→4ℓ and
H→WW*→ℓνℓν. The results are based on the complete
pp collision data sample recorded by the ATLAS experiment at
the CERN Large Hadron Collider at centre-of-mass energies of
s=7 TeV and s=8 TeV, corresponding to an integrated
luminosity of about 25 fb-1. Evidence for Higgs boson
production through vector-boson fusion is reported. Results
of combined fits probing Higgs boson couplings to fermions
and bosons, as well as anomalous contributions to
loop-induced production and decay modes, are presented. All
measurements are consistent with expectations for the
Standard Model Higgs boson. © 2013 CERN.},
Doi = {10.1016/j.physletb.2013.08.010},
Key = {fds308317}
}
@article{fds321280,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H},
Title = {Measurements of Higgs boson production and couplings in the
four-lepton channel in pp collisions at center-of-mass
energies of 7 and 8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.91.012006},
Abstract = {The final ATLAS Run 1 measurements of Higgs boson production
and couplings in the decay channel H → ZZ∗ →
l+l-l'+l'-, where l, l' = e or μ, are presented. These
measurements were performed using pp collision data
corresponding to integrated luminosities of 4.5 and 20.3
fb-1 at center-of-mass energies of 7 and 8 TeV,
respectively, recorded with the ATLAS detector at the LHC.
The H → ZZ∗ → 4l signal is observed with a
significance of 8.1 standard deviations, with an expectation
of 6.2 standard deviations, at mH = 125.36 GeV, the combined
ATLAS measurement of the Higgs boson mass from the H →
γγ and H → ZZ∗ → 4l channels. The production rate
relative to the Standard Model expectation, the signal
strength, is measured in four different production
categories in the H → ZZ∗ → 4l channel. The measured
signal strength, at this mass, and with all categories
combined, is 1.44+0.40-0.33. The signal strength for Higgs
boson production in gluon fusion or in association with tt
or bb pairs is found to be 1.7+0.5-0.4, while the signal
strength for vector-boson fusion combined with WH/ZH
associated production is found to be 0.3+1.6-0.9.},
Doi = {10.1103/PhysRevD.91.012006},
Key = {fds321280}
}
@article{fds375923,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Franco, L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
M and Bouquet, R and Marchiori, G and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
Gemmeren, P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Cui,
Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta,
D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Unal, M and Webb, AF and Huseynov, N and Agaras, MN and Bogavac, D and Bosman, M},
Title = {Measurements of Higgs boson production by gluon-gluon fusion
and vector-boson fusion using H→WW*→eνμν decays in pp
collisions at Formula Presented with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032005},
Abstract = {Higgs boson production via gluon-gluon fusion and
vector-boson fusion in proton-proton collisions is measured
in the H → W W * → e ν μ ν decay channel. The Large
Hadron Collider delivered proton-proton collisions at a
center-of-mass energy of 13 TeV between 2015 and 2018, which
were recorded by the ATLAS detector, corresponding to an
integrated luminosity of 139 fb - 1 . The total cross
sections for Higgs boson production by gluon-gluon fusion
and vector-boson fusion times the H → W W * branching
ratio are measured to be 12.0 ± 1.4 and 0.75 - 0.16 + 0.19
pb , respectively, in agreement with the Standard Model
predictions of 10.4 ± 0.6 and 0.81 ± 0.02 pb . Higgs boson
production is further characterized through measurements of
Simplified Template Cross Sections in a total of 11
kinematic fiducial regions.},
Doi = {10.1103/PhysRevD.108.032005},
Key = {fds375923}
}
@article{fds365394,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C and Arce, ATH and Arguin, JF},
Title = {Measurements of Higgs bosons decaying to bottom quarks from
vector boson fusion production with the ATLAS experiment at
√s=13TeV},
Journal = {European Physical Journal C},
Volume = {81},
Number = {6},
Year = {2021},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09192-8},
Abstract = {The paper presents a measurement of the Standard Model Higgs
Boson decaying to b-quark pairs in the vector boson fusion
(VBF) production mode. A sample corresponding to 126 fb - 1
of s=13TeV proton–proton collision data, collected with
the ATLAS experiment at the Large Hadron Collider, is
analyzed utilizing an adversarial neural network for event
classification. The signal strength, defined as the ratio of
the measured signal yield to that predicted by the Standard
Model for VBF Higgs production, is measured to be
0.95-0.36+0.38 , corresponding to an observed (expected)
significance of 2.6 (2.8) standard deviations from the
background only hypothesis. The results are additionally
combined with an analysis of Higgs bosons decaying to
b-quarks, produced via VBF in association with a
photon.},
Doi = {10.1140/epjc/s10052-021-09192-8},
Key = {fds365394}
}
@article{fds308640,
Author = {Abulencia, A and others},
Title = {Measurements of Inclusive W and Z Cross Sections in p anti-p
Collisions at $\sqrt{s} = 1.96$ TeV},
Journal = {J. Phys. G: Nucl. Part. Phys.},
Volume = {34},
Number = {12},
Pages = {2457-2544},
Publisher = {IOP Publishing},
Year = {2007},
url = {http://dx.doi.org/10.1088/0954-3899/34/12/001},
Abstract = {We report the first measurements of inclusive W and Z boson
cross-sections times the corresponding leptonic branching
ratios for p anti-p collisions at s**(1/2) = 1.96 TeV based
on the decays of the W and Z bosons into electrons and
muons. The data were recorded with the CDF II detector at
the Fermilab Tevatron and correspond to an integrated
luminosity of 72.0 +/- 4.3 pb-1. We test e-mu lepton
universality in W decays by measuring the ratio of the W -->
mu nu to W --> e nu cross sections and determine a value to
0.991 +/- 0.004(stat.) +/- 0.011(syst.) for the ratio of W -
l - nu couplings (g_mu/g_e). Since there is no sign of
non-universality, we combine our cross-section measurements
in the different lepton decay modes and obtain sigma_W x
Br(p anti-p --> W --> l nu) = 2.749 +/- 0.010(stat.) +/-
0.053(syst.) +/- 0.165(lum.) nb and sigma_gamma*/Z x BR(p
anti-p --> gamma*/Z --> ll) = 254.9 +/- 3.3(stat.) +/-
4.6(syst.) +/- 15.2(lum.) pb for dilepton pairs in the mass
range between 66 GeV/c2 and 116 GeV/c2. We compute the ratio
R of the W --> l nu to Z --> ll cross section taking all
correlations among channels into account and obtain R =
10.84 +/- 0.15(stat.) +/- 0.14(syst.) including a correction
for the virtual photon exchange component in our measured
gamma*/Z --> ll cross section. Based on the measured value
of R, we extract values for the W leptonic branching ratio,
Br(W --> l nu) = 0.1082 +/- 0.0022; the total width of the W
boson, Gamma(W) = 2092 +/- 42 MeV; and the ratio of W and Z
boson total widths, Gamma(W)/Gamma(Z) = 0.838 +/- 0.017. In
addition, we use our extracted value of Gamma(W) whose value
depends on various electroweak parameters and certain CKM
matrix elements to constrain the V_cs CKM matrix element,
|V_cs| = 0.976 +/- 0.030.},
Doi = {10.1088/0954-3899/34/12/001},
Key = {fds308640}
}
@article{fds321363,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, MF and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
A},
Title = {Measurements of jet vetoes and azimuthal decorrelations in
dijet events produced in [Formula: see text] collisions at
[Formula: see text] using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {11},
Pages = {3117},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3117-7},
Abstract = {Additional jet activity in dijet events is measured using
[Formula: see text] collisions at ATLAS at a centre-of-mass
energy of [Formula: see text], for jets reconstructed using
the [Formula: see text] algorithm with radius parameter
[Formula: see text]. This is done using variables such as
the fraction of dijet events without an additional jet in
the rapidity interval bounded by the dijet subsystem and
correlations between the azimuthal angles of the dijet s.
They are presented, both with and without a veto on
additional jet activity in the rapidity interval, as a
function of the scalar average of the transverse momenta of
the dijet s and of the rapidity interval size. The double
differential dijet cross section is also measured as a
function of the interval size and the azimuthal angle
between the dijet s. These variables probe differences in
the approach to resummation of large logarithms when
performing QCD calculations. The data are compared to
powheg, interfaced to the pythia 8 and herwig parton shower
generators, as well as to hej with and without interfacing
it to the ariadne parton shower generator. None of the
theoretical predictions agree with the data across the full
phase-space considered; however, powheg+pythia 8 and
hej+ariadne are found to provide the best agreement with the
data. These measurements use the full data sample collected
with the ATLAS detector in [Formula: see text][Formula: see
text] collisions at the LHC and correspond to integrated
luminosities of [Formula: see text] and [Formula: see text]
for data collected during 2010 and 2011,
respectively.},
Doi = {10.1140/epjc/s10052-014-3117-7},
Key = {fds321363}
}
@article{fds314180,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurements of normalized differential cross sections for
t¯t production in pp collisions at √(s) = 7 TeV using the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {October},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.90.072004},
Abstract = {Measurements of normalized differential cross sections for
top-quark pair production are presented as a function of the
top-quark transverse momentum, and of the mass, transverse
momentum, and rapidity of the t¯t system, in proton-proton
collisions at a center-of-mass energy of √s = 7 TeV. The
data set corresponds to an integrated luminosity of 4.6
fb-1, recorded in 2011 with the ATLAS detector at the CERN
Large Hadron Collider. Events are selected in the lepton +
jets channel, requiring exactly one lepton and at least four
jets with at least one of the jets tagged as originating
from a b-quark. The measured spectra are corrected for
detector efficiency and resolution effects and are compared
to several Monte Carlo simulations and theory calculations.
The results are in fair agreement with the predictions in a
wide kinematic range. Nevertheless, data distributions are
softer than predicted for higher values of the mass of the
t¯t system and of the top-quark transverse momentum. The
measurements can also discriminate among different sets of
parton distribution functions.},
Doi = {10.1103/PhysRevD.90.072004},
Key = {fds314180}
}
@article{fds375947,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Measurements of observables sensitive to colour reconnection
in tt¯ events with the ATLAS detector at √s=
13 TeV},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11479-x},
Abstract = {A measurement of observables sensitive to effects of colour
reconnection in top-quark pair-production events is
presented using 139 fb - 1 of 13 TeV proton–proton
collision data collected by the ATLAS detector at the LHC.
Events are selected by requiring exactly one isolated
electron and one isolated muon with opposite charge and two
or three jets, where exactly two jets are required to be
b-tagged. For the selected events, measurements are
presented for the charged-particle multiplicity, the scalar
sum of the transverse momenta of the charged particles, and
the same scalar sum in bins of charged-particle
multiplicity. These observables are unfolded to the
stable-particle level, thereby correcting for migration
effects due to finite detector resolution, acceptance and
efficiency effects. The particle-level measurements are
compared with different colour reconnection models in Monte
Carlo generators. These measurements disfavour some of the
colour reconnection models and provide inputs to future
optimisation of the parameters in Monte Carlo
generators.},
Doi = {10.1140/epjc/s10052-023-11479-x},
Key = {fds375947}
}
@article{fds365382,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Pereira, RA},
Title = {Measurements of sensor radiation damage in the ATLAS inner
detector using leakage currents},
Journal = {Journal of Instrumentation},
Volume = {16},
Number = {8},
Year = {2021},
Month = {August},
url = {http://dx.doi.org/10.1088/1748-0221/16/08/P08025},
Abstract = {Non-ionizing energy loss causes bulk damage to the silicon
sensors of the ATLAS pixel and strip detectors. This damage
has important implications for data-taking operations,
charged-particle track reconstruction, detector simulations,
and physics analysis. This paper presents simulations and
measurements of the leakage current in the ATLAS pixel
detector and semiconductor tracker as a function of location
in the detector and time, using data collected in Run 1
(2010–2012) and Run 2 (2015–2018) of the Large Hadron
Collider. The extracted fluence shows a much stronger
|z|-dependence in the innermost layers than is seen in
simulation. Furthermore, the overall fluence on the second
innermost layer is significantly higher than in simulation,
with better agreement in layers at higher radii. These
measurements are important for validating the simulation
models and can be used in part to justify safety factors for
future detector designs and interventions.},
Doi = {10.1088/1748-0221/16/08/P08025},
Key = {fds365382}
}
@article{fds321310,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurements of spin correlation in top-antitop quark events
from proton-proton collisions at √s =7 TeV using the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.90.112016},
Abstract = {Measurements of spin correlation in top quark pair
production are presented using data collected with the ATLAS
detector at the LHC with proton-proton collisions at a
center-of-mass energy of 7 TeV, corresponding to an
integrated luminosity of 4.6 fb-1. Events are selected in
final states with two charged leptons and at least two jets
and in final states with one charged lepton and at least
four jets. Four different observables sensitive to different
properties of the top quark pair production mechanism are
used to extract the correlation between the top and antitop
quark spins. Some of these observables are measured for the
first time. The measurements are in good agreement with the
Standard Model prediction at next-to-leading-order
accuracy.},
Doi = {10.1103/PhysRevD.90.112016},
Key = {fds321310}
}
@article{fds308411,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De
Cecco, S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier,
L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez,
T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi,
L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt,
M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
D and Weinberger, M and Wenzel, H and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T},
Title = {Measurements of the angular distributions in the decays
B→K(*)μ(+)μ(-) at CDF.},
Journal = {Physical review letters},
Volume = {108},
Number = {8},
Pages = {081807},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.108.081807},
Abstract = {We report an indirect search for nonstandard model physics
using the flavor-changing neutral current decays
B→K(*)μ(+)μ(-). We reconstruct the decays and measure
their angular distributions, as a function of
q(2)=M(μμ)(2)c(2), where M(μμ) is the dimuon mass, in
pp¯ collisions at √s=1.96 TeV using a data sample
corresponding to an integrated luminosity of 6.8 fb(-1). The
transverse polarization asymmetry A(T)(2) and the
time-reversal-odd charge-and-parity asymmetry A(im) are
measured for the first time, together with the K*
longitudinal polarization fraction F(L) and the muon
forward-backward asymmetry A(FB) for the decays
B(0)→K(*0)μ(+)μ(-) and B(+)→K(*+)μ(+)μ(-). The
B→K*μ(+)μ(-) forward-backward asymmetry in the most
sensitive kinematic regime, 1≤q(2)<6 GeV(2)/c(2), is
measured to be A(FB)=0.29(-0.23)(+0.20)(stat)±0.07(syst),
the most precise result to date. No deviations from the
standard model predictions are observed.},
Doi = {10.1103/physrevlett.108.081807},
Key = {fds308411}
}
@article{fds308392,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurements of the angular distributions of muons from Υ
decays in pp collisions at sqrt[s] = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {15},
Pages = {151802},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.108.151802},
Abstract = {The angular distributions of muons from Υ(1S,2S,3S) → μ+
μ- decays are measured using data from pp collisions at
sqrt[s] = 1.96 TeV corresponding to an integrated
luminosity of 6.7 fb(-1) and collected with the CDF II
detector at the Fermilab Tevatron. This analysis is the
first to report the full angular distributions as functions
of transverse momentum p(T) for Υ mesons in both the
Collins-Soper and s-channel helicity frames. This is also
the first measurement of the spin alignment of Υ(3S)
mesons. Within the kinematic range of Υ rapidity |y|<0.6
and p(T) up to 40 GeV/c, the angular distributions are
found to be nearly isotropic.},
Doi = {10.1103/physrevlett.108.151802},
Key = {fds308392}
}
@article{fds321180,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Measurements of the charge asymmetry in top-quark pair
production in the dilepton final state at s =8 TeV with the
ATLAS detector},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.032006},
Abstract = {Measurements of the top-antitop quark pair production charge
asymmetry in the dilepton channel, characterized by two
high-pT leptons (electrons or muons), are presented using
data corresponding to an integrated luminosity of 20.3 fb-1
from pp collisions at a center-of-mass energy s=8 TeV
collected with the ATLAS detector at the Large Hadron
Collider at CERN. Inclusive and differential measurements as
a function of the invariant mass, transverse momentum, and
longitudinal boost of the tt system are performed both in
the full phase space and in a fiducial phase space closely
matching the detector acceptance. Two observables are
studied: ACℓℓ based on the selected leptons and ACtt
based on the reconstructed tt final state. The inclusive
asymmetries are measured in the full phase space to be
ACℓℓ=0.008±0.006 and ACtt=0.021±0.016, which are in
agreement with the Standard Model predictions of
ACℓℓ=0.0064±0.0003 and ACtt=0.0111±0.0004.},
Doi = {10.1103/PhysRevD.94.032006},
Key = {fds321180}
}
@article{fds365427,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
C},
Title = {Measurements of the Higgs boson inclusive and differential
fiducial cross sections in the 4 ℓ decay channel at √s =
13 TeV},
Journal = {European Physical Journal C},
Volume = {80},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8223-0},
Abstract = {Inclusive and differential fiducial cross sections of the
Higgs boson are measured in the H→ ZZ∗→ 4 ℓ (ℓ= e,
μ) decay channel. The results are based on proton−proton
collision data produced at the Large Hadron Collider at a
centre-of-mass energy of 13 TeV and recorded by the ATLAS
detector from 2015 to 2018, equivalent to an integrated
luminosity of 139 fb - 1. The inclusive fiducial cross
section for the H→ ZZ∗→ 4 ℓ process is measured to
be σfid= 3.28 ± 0.32 fb, in agreement with the Standard
Model prediction of σfid , SM= 3.41 ± 0.18 fb.
Differential fiducial cross sections are measured for a
variety of observables which are sensitive to the production
and decay of the Higgs boson. All measurements are in
agreement with the Standard Model predictions. The results
are used to constrain anomalous Higgs boson interactions
with Standard Model particles.},
Doi = {10.1140/epjc/s10052-020-8223-0},
Key = {fds365427}
}
@article{fds321179,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Measurements of the Higgs boson production and decay rates
and constraints on its couplings from a combined ATLAS and
CMS analysis of the LHC pp collision data at √s = 7 and 8
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)045},
Abstract = {Combined ATLAS and CMS measurements of the Higgs boson
production and decay rates, as well as constraints on its
couplings to vector bosons and fermions, are presented. The
combination is based on the analysis of five production
processes, namely gluon fusion, vector boson fusion, and
associated production with a W or a Z boson or a pair of top
quarks, and of the six decay modes H → ZZ, W W, γγ,
ττ, bb, and μμ. All results are reported assuming a
value of 125.09 GeV for the Higgs boson mass, the result of
the combined measurement by the ATLAS and CMS experiments.
The analysis uses the CERN LHC proton-proton collision data
recorded by the ATLAS and CMS experiments in 2011 and 2012,
corresponding to integrated luminosities per experiment of
approximately 5 fb−1 at √s = 7 TeV and 20 fb−1 at √s
= 8 TeV. The Higgs boson production and decay rates measured
by the two experiments are combined within the context of
three generic parameterisations: two based on cross sections
and branching fractions, and one on ratios of coupling
modifiers. Several interpretations of the measurements with
more model-dependent parameterisations are also given. The
combined signal yield relative to the Standard Model
prediction is measured to be 1.09 ± 0.11. The combined
measurements lead to observed significances for the vector
boson fusion production process and for the H → ττ decay
of 5.4 and 5.5 standard deviations, respectively. The data
are consistent with the Standard Model predictions for all
parameterisations considered.},
Doi = {10.1007/JHEP08(2016)045},
Key = {fds321179}
}
@article{fds365381,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Measurements of the inclusive and differential production
cross sections of a top-quark–antiquark pair in
association with a Z boson at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {8},
Year = {2021},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09439-4},
Abstract = {Measurements of both the inclusive and differential
production cross sections of a top-quark–antiquark pair in
association with a Z boson (tt¯ Z) are presented. The
measurements are performed by targeting final states with
three or four isolated leptons (electrons or muons) and are
based on s=13 TeV proton–proton collision data with an
integrated luminosity of 139 fb - 1, recorded from 2015 to
2018 with the ATLAS detector at the CERN Large Hadron
Collider. The inclusive cross section is measured to be
σtt¯Z= 0.99 ± 0.05 (stat.) ±0.08 (syst.) pb, in
agreement with the most precise theoretical predictions. The
differential measurements are presented as a function of a
number of kinematic variables which probe the kinematics of
the tt¯ Z system. Both absolute and normalised differential
cross-section measurements are performed at particle and
parton levels for specific fiducial volumes and are compared
with theoretical predictions at different levels of
precision, based on a χ2/ ndf and p value computation.
Overall, good agreement is observed between the unfolded
data and the predictions.},
Doi = {10.1140/epjc/s10052-021-09439-4},
Key = {fds365381}
}
@article{fds321268,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
Title = {Measurements of the Nuclear Modification Factor for Jets in
Pb+Pb Collisions at √(s)NN]=2.76 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {7},
Pages = {072302},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.114.072302},
Abstract = {Measurements of inclusive jet production are performed in pp
and Pb+Pb collisions at √(s)NN=2.76 TeV with the
ATLAS detector at the LHC, corresponding to integrated
luminosities of 4.0 and 0.14 nb(-1), respectively. The
jets are identified with the anti-k(t) algorithm with R=0.4,
and the spectra are measured over the kinematic range of jet
transverse momentum 32<p(T)<500 GeV and absolute
rapidity |y|<2.1 and as a function of collision centrality.
The nuclear modification factor R(AA) is evaluated, and jets
are found to be suppressed by approximately a factor of 2 in
central collisions compared to pp collisions. The R(AA)
shows a slight increase with p(T) and no significant
variation with rapidity.},
Doi = {10.1103/physrevlett.114.072302},
Key = {fds321268}
}
@article{fds314157,
Author = {Aaltonen, T and González, BÃ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester,
WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang,
YC},
Title = {Measurements of the properties of Λc(2595),
Λc(2625), Σc(2455), and Σ
c(2520) baryons},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {84},
Number = {1},
Year = {2011},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.84.012003},
Abstract = {We report measurements of the resonance properties of Λ
c(2595)+ and Λc(2625)+ baryons in their decays to
Λc+π+π- as well as Σc(2455)++,0 and Σ c(2520)++,0
baryons in their decays to Λc+π± final states. These
measurements are performed using data corresponding to
5.2fb-1 of integrated luminosity from pp̄ collisions at
√s=1.96TeV, collected with the CDF II detector at the
Fermilab Tevatron. Exploiting the largest available charmed
baryon sample, we measure masses and decay widths with
uncertainties comparable to the world averages for Σc
states, and significantly smaller uncertainties than the
world averages for excited Λc+ states. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevD.84.012003},
Key = {fds314157}
}
@article{fds375951,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V},
Title = {Measurements of the suppression and correlations of dijets
in Pb+Pb collisions at√sNN = 5.02
TeV},
Journal = {Physical Review C},
Volume = {107},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevC.107.054908},
Abstract = {Studies of the correlations of the two highest transverse
momentum (leading) jets in individual Pb+Pb collision events
can provide information about the mechanism of jet quenching
by the hot and dense matter created in such collisions. In
Pb+Pb and pp collisions at√sNN = 5.02 TeV, measurements of
the leading dijet transverse momentum (pT) correlations are
presented. Additionally, measurements in Pb+Pb collisions of
the dijet pair nuclear modification factors projected along
leading and subleading jet pT are made. The measurements are
performed using the ATLAS detector at the LHC with 260
pb−1 of pp data collected in 2017 and 2.2 nb−1 of Pb+Pb
data collected in 2015 and 2018. An unfolding procedure is
applied to the two-dimensional leading and subleading jet pT
distributions to account for experimental effects in the
measurement of both jets. Results are provided for dijets
with leading jet pT greater than 100 GeV. Measurements of
the dijet-yield-normalized xJ distributions in Pb+Pb
collisions show an increased fraction of imbalanced jets
compared to pp collisions; these measurements are in
agreement with previous measurements of the same quantity at
2.76 TeV in the overlapping kinematic range. Measurements of
the absolutely normalized dijet rate in Pb+Pb and pp
collisions are also presented, and show that balanced dijets
are significantly more suppressed than imbalanced dijets in
Pb+Pb collisions. It is observed in the measurements of the
pair nuclear modification factors that the subleading jets
are significantly suppressed relative to leading jets with
pT between 100 and 316 GeV for all centralities in Pb+Pb
collisions.},
Doi = {10.1103/PhysRevC.107.054908},
Key = {fds375951}
}
@article{fds375922,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Guillemin, T and Hryn'ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis,
DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Sanchez
Pineda, A and Sauvan, E and Selem, L and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori, G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang, R and Zhang, J and Berlendis,
S and Cheu, E and Cui, Z and Ghosh, A and Johns, KA and Lampl, W and Lindley,
RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou,
H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai,
G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost, M and Unal, M and Huseynov, N},
Title = {Measurements of the suppression and correlations of dijets
in Xe+Xe collisions at Formula Presented
TeV},
Journal = {Physical Review C},
Volume = {108},
Number = {2},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevC.108.024906},
Abstract = {Measurements of the suppression and correlations of dijets
is performed using 3 µ b − 1 of Xe+Xe data at s N N =
5.44 TeV collected with the ATLAS detector at the CERN Large
Hadron Collider. Dijets with jets reconstructed using the R
= 0.4 anti- k t algorithm are measured differentially in jet
p T over the range of 32 to 398 GeV and the centrality of
the collisions. Significant dijet momentum imbalance is
found in the most central Xe+Xe collisions, which decreases
in more peripheral collisions. Results from the measurement
of per-pair normalized and absolutely normalized dijet p T
balance are compared with previous Pb + Pb measurements at s
N N = 5.02 TeV. The differences between the dijet
suppression in Xe+Xe and Pb + Pb are further quantified by
the ratio of pair nuclear-modification factors. The results
are found to be consistent with those measured in Pb + Pb
data when compared in classes of the same event activity and
when taking into account the difference between the
center-of-mass energies of the initial parton scattering
process in Xe+Xe and Pb + Pb collisions. These results
should provide input for a better understanding of the role
of energy density, system size, path length, and
fluctuations in the parton energy loss.},
Doi = {10.1103/PhysRevC.108.024906},
Key = {fds375922}
}
@article{fds314190,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurements of the top quark branching ratios into channels
with leptons and quarks with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.92.072005},
Abstract = {Measurements of the branching ratios of top quark decays
into leptons and jets using events with tt (top antitop)
pairs are reported. Events were recorded with the ATLAS
detector at the LHC in pp collisions at a center-of-mass
energy of 7 TeV. The collected data sample corresponds to an
integrated luminosity of 4.6 fb-1. The measured top quark
branching ratios agree with the Standard Model predictions
within the measurement uncertainties of a few
percent.},
Doi = {10.1103/PhysRevD.92.072005},
Key = {fds314190}
}
@article{fds308371,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurements of the top-quark mass and the tt cross section
in the hadronic τ+jets decay channel at sqrt[s] = 1.96
TeV.},
Journal = {Physical review letters},
Volume = {109},
Number = {19},
Pages = {192001},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.109.192001},
Abstract = {We present the first direct measurement of the top-quark
mass using tt events decaying in the hadronic τ+jets decay
channel. Using data corresponding to an integrated
luminosity of 2.2 fb(-1) collected by the CDF II detector in
pp collisions at sqrt[s] = 1.96 TeV at the Fermilab
Tevatron, we measure the tt cross section, σ(tt), and the
top-quark mass, M(top). We extract M(top) from a likelihood
based on per-event probabilities calculated with
leading-order signal and background matrix elements. We
measure σ(tt) = 8.8 ± 3.3(stat) ± 2.2(syst) pb and M(top)
= 172.7 ± 9.3(stat) ± 3.7(syst) GeV/c(2).},
Doi = {10.1103/physrevlett.109.192001},
Key = {fds308371}
}
@article{fds308490,
Author = {Aaltonen, and T, and others},
Title = {Measurements of the top-quark mass using charged particle
tracking},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {3},
Pages = {032002},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.032002},
Abstract = {http://arxiv.org/abs/0910.0969},
Doi = {10.1103/PhysRevD.81.032002},
Key = {fds308490}
}
@article{fds321228,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek,
P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura,
AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro,
F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton,
AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista,
SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G},
Title = {Measurements of the Total and Differential Higgs Boson
Production Cross Sections Combining the H→γγ and
H→ZZ^{*}→4ℓ Decay Channels at sqrt[s]=8 TeV with
the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {115},
Number = {9},
Pages = {091801},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.115.091801},
Abstract = {Measurements of the total and differential cross sections of
Higgs boson production are performed using 20.3 fb^{-1}
of pp collisions produced by the Large Hadron Collider at a
center-of-mass energy of sqrt[s]=8 TeV and recorded by
the ATLAS detector. Cross sections are obtained from
measured H→γγ and H→ZZ^{*}→4ℓ event yields, which
are combined accounting for detector efficiencies, fiducial
acceptances, and branching fractions. Differential cross
sections are reported as a function of Higgs boson
transverse momentum, Higgs boson rapidity, number of jets in
the event, and transverse momentum of the leading jet. The
total production cross section is determined to be
σ_{pp→H}=33.0±5.3 (stat)±1.6 (syst) pb. The
measurements are compared to state-of-the-art
predictions.},
Doi = {10.1103/physrevlett.115.091801},
Key = {fds321228}
}
@article{fds321286,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
M},
Title = {Measurements of the [Formula: see text] production cross
sections in association with jets with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {2},
Pages = {82},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3262-7},
Abstract = {This paper presents cross sections for the production of a
[Formula: see text] boson in association with jets, measured
in proton-proton collisions at [Formula: see text] with the
ATLAS experiment at the large hadron collider. With an
integrated luminosity of [Formula: see text], this data set
allows for an exploration of a large kinematic range,
including jet production up to a transverse momentum of
[Formula: see text] and multiplicities up to seven
associated jets. The production cross sections for [Formula:
see text] bosons are measured in both the electron and muon
decay channels. Differential cross sections for many
observables are also presented including measurements of the
jet observables such as the rapidities and the transverse
momenta as well as measurements of event observables such as
the scalar sums of the transverse momenta of the jets. The
measurements are compared to numerous QCD predictions
including next-to-leading-order perturbative calculations,
resummation calculations and Monte Carlo
generators.},
Doi = {10.1140/epjc/s10052-015-3262-7},
Key = {fds321286}
}
@article{fds321158,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerny, K and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
Title = {Measurements of top-quark pair differential cross-sections
in the lepton+jets channel in pp collisions at
[Formula: see text] using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {10},
Pages = {538},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4366-4},
Abstract = {Measurements of normalized differential cross-sections of
top-quark pair production are presented as a function of
the top-quark, [Formula: see text] system and event-level
kinematic observables in proton-proton collisions at
a centre-of-mass energy of [Formula: see text]. The
observables have been chosen to emphasize the [Formula: see
text] production process and to be sensitive to effects of
initial- and final-state radiation, to the different parton
distribution functions, and to non-resonant processes and
higher-order corrections. The dataset corresponds to an
integrated luminosity of 20.3 fb[Formula: see text],
recorded in 2012 with the ATLAS detector at the CERN Large
Hadron Collider. Events are selected in the lepton+jets
channel, requiring exactly one charged lepton and at least
four jets with at least two of the jets tagged as
originating from a <i>b</i>-quark. The measured spectra are
corrected for detector effects and are compared to several
Monte Carlo simulations. The results are in fair agreement
with the predictions over a wide kinematic range.
Nevertheless, most generators predict a harder top-quark
transverse momentum distribution at high values than what is
observed in the data. Predictions beyond NLO accuracy
improve the agreement with data at high top-quark transverse
momenta. Using the current settings and parton distribution
functions, the rapidity distributions are not well modelled
by any generator under consideration. However, the level of
agreement is improved when more recent sets of parton
distribution functions are used.},
Doi = {10.1140/epjc/s10052-016-4366-4},
Key = {fds321158}
}
@article{fds365430,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud,
AA and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai,
X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Estevez, MA and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP},
Title = {Measurements of top-quark pair spin correlations in the eμ
channel at √s=13 TeV using pp collisions in the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {8},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8181-6},
Abstract = {A measurement of observables sensitive to spin correlations
in tt¯ production is presented, using 36.1 fb - 1 of pp
collision data at s=13 TeV recorded with the ATLAS detector
at the Large Hadron Collider. Differential cross-sections
are measured in events with exactly one electron and one
muon with opposite-sign electric charge as a function of the
azimuthal opening angle and the absolute difference in
pseudorapidity between the electron and muon candidates in
the laboratory frame. The azimuthal opening angle is also
measured as a function of the invariant mass of the tt¯
system. The measured differential cross-sections are
compared to predictions by several NLO Monte Carlo
generators and fixed-order calculations. The observed degree
of spin correlation is somewhat higher than predicted by the
generators used. The data are consistent with the prediction
of one of the fixed-order calculations at NLO, but agree
less well with higher-order predictions. Using these
leptonic observables, a search is performed for pair
production of supersymmetric top squarks decaying into
Standard Model top quarks and light neutralinos. Top squark
masses between 170 and 230 GeV are largely excluded at the
95% confidence level for kinematically allowed values of the
neutralino mass.},
Doi = {10.1140/epjc/s10052-020-8181-6},
Key = {fds365430}
}
@article{fds365393,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Measurements of W + W −+ ≥ 1 jet
production cross-sections in pp collisions at √s = 13 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {6},
Year = {2021},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2021)003},
Abstract = {Fiducial and differential cross-section measurements of
W+W− production in association with at least one hadronic
jet are presented. These measurements are sensitive to the
properties of electroweak-boson self-interactions and
provide a test of perturbative quantum chromodynamics and
the electroweak theory. The analysis is performed using
proton-proton collision data collected at s = 13 TeV with
the ATLAS experiment, corresponding to an integrated
luminosity of 139 fb−1. Events are selected with exactly
one oppositely charged electron-muon pair and at least one
hadronic jet with a transverse momentum of pT> 30 GeV and a
pseudorapidity of |η| < 4.5. After subtracting the
background contributions and correcting for detector
effects, the jet-inclusive W+W−+ ≥ 1 jet fiducial
cross-section and W+W−+ jets differential cross-sections
with respect to several kinematic variables are measured.
These measurements include leptonic quantities, such as the
lepton transverse momenta and the transverse mass of the
W+W− system, as well as jet-related observables such as
the leading jet transverse momentum and the jet
multiplicity. Limits on anomalous triple-gauge-boson
couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous
amplitude is enhanced. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP06(2021)003},
Key = {fds365393}
}
@article{fds375919,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
Bella, L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Measurements of W+W- production in
decay topologies inspired by searches for electroweak
supersymmetry},
Journal = {European Physical Journal C},
Volume = {83},
Number = {8},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11508-9},
Abstract = {This paper presents a measurement of fiducial and
differential cross-sections for W+W- production in
proton–proton collisions at s=13 TeV with the ATLAS
experiment at the Large Hadron Collider using a dataset
corresponding to an integrated luminosity of 139 fb - 1 .
Events with exactly one electron, one muon and no hadronic
jets are studied. The fiducial region in which the
measurements are performed is inspired by searches for the
electroweak production of supersymmetric charginos decaying
to two-lepton final states. The selected events have
moderate values of missing transverse momentum and the
‘stransverse mass’ variable mT2 , which is widely used
in searches for supersymmetry at the LHC. The ranges of
these variables are chosen so that the acceptance is
enhanced for direct W+W- production and suppressed for
production via top quarks, which is treated as a background.
The fiducial cross-section and particle-level differential
cross-sections for six variables are measured and compared
with two theoretical SM predictions from perturbative QCD
calculations.},
Doi = {10.1140/epjc/s10052-023-11508-9},
Key = {fds375919}
}
@article{fds365412,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Measurements of WH and ZH production in the H→ bb¯ decay
channel in pp collisions at 13Te with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {2},
Year = {2021},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08677-2},
Abstract = {Measurements of the Standard Model Higgs boson decaying into
a bb¯ pair and produced in association with a W or Z boson
decaying into leptons, using proton–proton collision data
collected between 2015 and 2018 by the ATLAS detector, are
presented. The measurements use collisions produced by the
Large Hadron Collider at a centre-of-mass energy of s=13Te,
corresponding to an integrated luminosity of 139fb-1. The
production of a Higgs boson in association with a W or Z
boson is established with observed (expected) significances
of 4.0 (4.1) and 5.3 (5.1) standard deviations,
respectively. Cross-sections of associated production of a
Higgs boson decaying into bottom quark pairs with an
electroweak gauge boson, W or Z, decaying into leptons are
measured as a function of the gauge boson transverse
momentum in kinematic fiducial volumes. The cross-section
measurements are all consistent with the Standard Model
expectations, and the total uncertainties vary from 30% in
the high gauge boson transverse momentum regions to 85% in
the low regions. Limits are subsequently set on the
parameters of an effective Lagrangian sensitive to
modifications of the WH and ZH processes as well as the
Higgs boson decay into bb¯.},
Doi = {10.1140/epjc/s10052-020-08677-2},
Key = {fds365412}
}
@article{fds316857,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A},
Title = {Measurements of W±Z production cross sections in pp
collisions at s =8 TeV with the ATLAS detector and limits on
anomalous gauge boson self-couplings},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {93},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {May},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.93.092004},
Abstract = {This paper presents measurements of W±Z production in pp
collisions at a center-of-mass energy of 8 TeV. The gauge
bosons are reconstructed using their leptonic decay modes
into electrons and muons. The data were collected in 2012 by
the ATLAS experiment at the Large Hadron Collider and
correspond to an integrated luminosity of 20.3 fb-1. The
measured inclusive cross section in the detector fiducial
region is σW±Z→ ′ν=35.1±0.9(stat)±0.8(sys)±0.8(lumi)
fb, for one leptonic decay channel. In comparison, the
next-to-leading-order Standard Model expectation is
30.0±2.1 fb. Cross sections for W+Z and W-Z production and
their ratio are presented as well as differential cross
sections for several kinematic observables. Limits on
anomalous triple gauge boson couplings are derived from the
transverse mass spectrum of the W±Z system. From the
analysis of events with a W and a Z boson associated with
two or more forward jets an upper limit at 95% confidence
level on the W±Z scattering cross section of 0.63 fb, for
each leptonic decay channel, is established, while the
Standard Model prediction at next-to-leading order is
0.13±0.01 fb. Limits on anomalous quartic gauge boson
couplings are also extracted.},
Doi = {10.1103/PhysRevD.93.092004},
Key = {fds316857}
}
@article{fds308328,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Measurements of Wγ and Zγ production in pp collisions at
√s=7 TeV with the ATLAS detector at the
LHC},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.87.112003},
Abstract = {The integrated and differential fiducial cross sections for
the production of a W or Z boson in association with a
high-energy photon are measured using pp collisions at
√s=7 TeV. The analyses use a data sample with an
integrated luminosity of 4.6 fb-1 collected by the ATLAS
detector during the 2011 LHC data-taking period. Events are
selected using leptonic decays of the W and Z bosons
[W(eν,μν) and Z(e+e-, μ+μ-,νν¯)] with the
requirement of an associated isolated photon. The data are
used to test the electroweak sector of the Standard Model
and search for evidence for new phenomena. The measurements
are used to probe the anomalous WWγ, ZZγ, and Zγγ
triple-gauge-boson couplings and to search for the
production of vector resonances decaying to Zγ and Wγ. No
deviations from Standard Model predictions are observed and
limits are placed on anomalous triple-gauge-boson couplings
and on the production of new vector meson
resonances.},
Doi = {10.1103/PhysRevD.87.112003},
Key = {fds308328}
}
@article{fds321194,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Measurements of Zγ and Zγγ production in pp collisions at
s =8 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112002},
Abstract = {The production of Z bosons with one or two isolated
high-energy photons is studied using pp collisions at s=8
TeV. The analyses use a data sample with an integrated
luminosity of 20.3 fb-1 collected by the ATLAS detector
during the 2012 LHC data taking. The Zγ and Zγγ
production cross sections are measured with leptonic (e+e-,
μ+μ-, νν) decays of the Z boson, in extended fiducial
regions defined in terms of the lepton and photon
acceptance. They are then compared to cross-section
predictions from the Standard Model, where the sources of
the photons are radiation off initial-state quarks and
radiative Z-boson decay to charged leptons, and from
fragmentation of final-state quarks and gluons into photons.
The yields of events with photon transverse energy ET>250
GeV from +-γ events and with ET>400 GeV from ννγ events
are used to search for anomalous triple gauge-boson
couplings ZZγ and Zγγ. The yields of events with diphoton
invariant mass mγγ>200 GeV from +-γγ events and with
mγγ>300 GeV from ννγγ events are used to search for
anomalous quartic gauge-boson couplings ZZγγ and Zγγγ.
No deviations from Standard Model predictions are observed
and limits are placed on parameters used to describe
anomalous triple and quartic gauge-boson
couplings.},
Doi = {10.1103/PhysRevD.93.112002},
Key = {fds321194}
}
@article{fds365365,
Author = {Bauer, M and Neubert, M},
Title = {Minimal Leptoquark Explanation for the R_{D^{(*)}}, R_{K},
and (g-2)_{μ} Anomalies.},
Journal = {Physical review letters},
Volume = {116},
Number = {14},
Pages = {141802},
Year = {2016},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.116.141802},
Abstract = {We show that by adding a single new scalar particle to the
standard model, a TeV-scale leptoquark with the quantum
numbers of a right-handed down quark, one can explain in a
natural way three of the most striking anomalies of particle
physics: the violation of lepton universality in B[over
¯]→K[over ¯]ℓ^{+}ℓ^{-} decays, the enhanced B[over
¯]→D^{(*)}τν[over ¯] decay rates, and the anomalous
magnetic moment of the muon. Constraints from other
precision measurements in the flavor sector can be satisfied
without fine-tuning. Our model predicts enhanced B[over
¯]→K[over ¯]^{(*)}νν[over ¯] decay rates and a
new-physics contribution to B_{s}-B[over ¯]_{s} mixing
close to the current central fit value.},
Doi = {10.1103/physrevlett.116.141802},
Key = {fds365365}
}
@article{fds331631,
Author = {Collaboration, DAEACDF},
Title = {Momentum distribution of charged particles in jets in dijet
events in pp-bar collisions at sqrt[s]=1.8 TeV and
comparisons to perturbative QCD predictions},
Journal = {Physical Review},
Volume = {D68},
Number = {1},
Pages = {012003},
Publisher = {American Physical Society (APS)},
Year = {2003},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.68.012003},
Abstract = {Inclusive momentum distributions of charged particles in
restricted cones around jet axes were measured in dijet
events with invariant dijet masses in the range 80 to
600 GeV/c2. Events were produced at the Fermilab Tevatron
in pp-bar collisions with a center of mass energy of 1.8 TeV
and recorded by the Collider Detector at Fermilab. The
results were compared to perturbative QCD calculations
carried out in the framework of the modified leading log
approximation (MLLA) and assuming local parton-hadron
duality. It was shown that the data follow theoretical
predictions quite well over the whole range of the jet
energies included in this analysis. We extracted the MLLA
cutoff scale Qeff and found a value of 230±40 MeV. The
theoretical prediction of Ejetsin theta c scaling, where
theta c is the cone opening angle, was experimentally
observed for the first time. From the MLLA fits to the data,
two more parameters were extracted: the ratio of parton
multiplicities in gluon and quark jets, r=Ng-jetpartons/Nq-jetpartons=1.9±0.5,
and the ratio of the number of charged hadrons to the number
of predicted partons in a jet, KchargedLPHD=Nchargedhadrons/Npartons=0.56±0.10.},
Doi = {10.1103/PhysRevD.68.012003},
Key = {fds331631}
}
@article{fds321344,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Monitoring and data quality assessment of the ATLAS liquid
argon calorimeter},
Journal = {Journal of Instrumentation},
Volume = {9},
Number = {7},
Pages = {P07024-P07024},
Publisher = {IOP Publishing},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1088/1748-0221/9/07/P07024},
Abstract = {The liquid argon calorimeter is a key component of the ATLAS
detector installed at the CERN Large Hadron Collider. The
primary purpose of this calorimeter is the measurement of
electron and photon kinematic properties. It also provides a
crucial input for measuring jets and missing transverse
momentum. An advanced data monitoring procedure was designed
to quickly identify issues that would affect detector
performance and ensure that only the best quality data are
used for physics analysis. This article presents the
validation procedure developed during the 2011 and 2012 LHC
data-taking periods, in which more than 98% of the
proton-proton luminosity recorded by ATLAS at a
centre-of-mass energy of 7-8 TeV had calorimeter data
quality suitable for physics analysis. © CERN 2014 for the
benefit of the ATLAS collaboration.},
Doi = {10.1088/1748-0221/9/07/P07024},
Key = {fds321344}
}
@article{fds308345,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
OK and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer,
F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro,
A},
Title = {Multi-channel search for squarks and gluinos in [Formula:
see text]pp collisions with the ATLAS detector at the
LHC.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {3},
Pages = {2362},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2362-5},
Abstract = {A search for supersymmetric particles in final states with
zero, one, and two leptons, with and without jets identified
as originating from <i>b</i>-quarks, in 4.7 fb<sup>-1</sup>
of [Formula: see text]<i>pp</i> collisions produced by the
Large Hadron Collider and recorded by the ATLAS detector is
presented. The search uses a set of variables carrying
information on the event kinematics transverse and parallel
to the beam line that are sensitive to several topologies
expected in supersymmetry. Mutually exclusive final states
are defined, allowing a combination of all channels to
increase the search sensitivity. No deviation from the
Standard Model expectation is observed. Upper limits at
95 % confidence level on visible cross-sections for the
production of new particles are extracted. Results are
interpreted in the context of the constrained minimal
supersymmetric extension to the Standard Model and in
supersymmetry-inspired models with diverse,
high-multiplicity final states.},
Doi = {10.1140/epjc/s10052-013-2362-5},
Key = {fds308345}
}
@article{fds365389,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Muon reconstruction and identification efficiency in ATLAS
using the full Run 2 pp collision data set at √s=13
TeV},
Journal = {European Physical Journal C},
Volume = {81},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09233-2},
Abstract = {This article documents the muon reconstruction and
identification efficiency obtained by the ATLAS experiment
for 139 fb - 1 of pp collision data at s=13 TeV collected
between 2015 and 2018 during Run 2 of the LHC. The increased
instantaneous luminosity delivered by the LHC over this
period required a reoptimisation of the criteria for the
identification of prompt muons. Improved and newly developed
algorithms were deployed to preserve high muon
identification efficiency with a low misidentification rate
and good momentum resolution. The availability of large
samples of Z→ μμ and J/ ψ→ μμ decays, and the
minimisation of systematic uncertainties, allows the
efficiencies of criteria for muon identification, primary
vertex association, and isolation to be measured with an
accuracy at the per-mille level in the bulk of the phase
space, and up to the percent level in complex kinematic
configurations. Excellent performance is achieved over a
range of transverse momenta from 3 GeV to several hundred
GeV, and across the full muon detector acceptance of | η| <
2.7.},
Doi = {10.1140/epjc/s10052-021-09233-2},
Key = {fds365389}
}
@article{fds321361,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella,
G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat,
P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiarella,
V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
RN},
Title = {Muon reconstruction efficiency and momentum resolution of
the ATLAS experiment in proton-proton collisions at
[Formula: see text] TeV in 2010.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {9},
Pages = {3034},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3034-9},
Abstract = {This paper presents a study of the performance of the muon
reconstruction in the analysis of proton-proton collisions
at [Formula: see text] TeV at the LHC, recorded by the
ATLAS detector in 2010. This performance is described in
terms of reconstruction and isolation efficiencies and
momentum resolutions for different classes of reconstructed
muons. The results are obtained from an analysis of
[Formula: see text] meson and [Formula: see text] boson
decays to dimuons, reconstructed from a data sample
corresponding to an integrated luminosity of 40 pb[Formula:
see text]. The measured performance is compared to Monte
Carlo predictions and deviations from the predicted
performance are discussed.},
Doi = {10.1140/epjc/s10052-014-3034-9},
Key = {fds321361}
}
@article{fds316860,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi,
S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier,
S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro,
R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero,
J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {Muon reconstruction performance of the ATLAS detector in
proton-proton collision data at [Formula: see
text]=13 TeV.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {292},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4120-y},
Abstract = {This article documents the performance of the ATLAS muon
identification and reconstruction using the LHC dataset
recorded at [Formula: see text] TeV in 2015. Using a large
sample of [Formula: see text] and [Formula: see text] decays
from 3.2 fb[Formula: see text] of <i>pp</i> collision data,
measurements of the reconstruction efficiency, as well as of
the momentum scale and resolution, are presented and
compared to Monte Carlo simulations. The reconstruction
efficiency is measured to be close to [Formula: see text]
over most of the covered phase space ([Formula: see text]
and [Formula: see text] GeV). The isolation efficiency
varies between 93 and [Formula: see text] depending on the
selection applied and on the momentum of the muon. Both
efficiencies are well reproduced in simulation. In the
central region of the detector, the momentum resolution is
measured to be [Formula: see text] ([Formula: see text]) for
muons from [Formula: see text] ([Formula: see text]) decays,
and the momentum scale is known with an uncertainty of
[Formula: see text]. In the region [Formula: see text], the
[Formula: see text] resolution for muons from [Formula: see
text] decays is [Formula: see text] while the precision of
the momentum scale for low-[Formula: see text] muons from
[Formula: see text] decays is about [Formula: see
text].},
Doi = {10.1140/epjc/s10052-016-4120-y},
Key = {fds316860}
}
@article{fds375911,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez,
MA and Fernandez, AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen,
T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez,
O and Arnold, H and Tame, ZPA and Artoni, G and Asada, H and Asai, K and Asai,
S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi,
S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakos, E and Gupta, DB and Balasubramanian, R and Baldin,
EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas,
WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits,
M-S and Barklow, T and Baron, P and Moreno, DAB and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Navarro, LB and Barreiro, F and da
Costa, JBG and Barron, U and Teixeira, MGB and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Hurrell, LTB and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Kuutmann, EB and Berger, N and Bergmann, B and Beringer, J and Bernardi,
G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta,
P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Sola, JDB and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and de Renstrom, PAB and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Bunka, AT and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr,
JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Vazquez, CJB and Buzykaev, AR and Cabras, G and Urbán,
SC and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea,
G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti,
M and Toro, RC and Camarda, S and Munoz, DC and Camarri, P and Camerlingo,
MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Bret, MC and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron,
S and Carquin, E and Carrá, S and Carratta, G and Argos, FC and Carter,
JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Garcia, LC and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Moursli, RCE and Cheu, E and Cheung, K and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi,
K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A},
Title = {New techniques for jet calibration with the ATLAS
detector},
Journal = {The European Physical Journal C},
Volume = {83},
Number = {8},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11837-9},
Abstract = {<jats:title>Abstract</jats:title><jats:p>A determination of
the jet energy scale is presented using proton–proton
collision data with a centre-of-mass energy of
<jats:inline-formula><jats:alternatives><jats:tex-math>$$\sqrt{s}=13$$</jats:tex-math>??
<mml:mrow> <mml:msqrt> <mml:mi>s</mml:mi> </mml:msqrt>
<mml:mo>=</mml:mo> <mml:mn>13</mml:mn> </mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula> TeV,
corresponding to an integrated luminosity of 140
fb<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{-1}$$</jats:tex-math>??
<mml:msup> <mml:mrow /> <mml:mrow> <mml:mo>-</mml:mo>
<mml:mn>1</mml:mn> </mml:mrow> </mml:msup>
</mml:math></jats:alternatives></jats:inline-formula>
collected using the ATLAS detector at the LHC. Jets are
reconstructed using the ATLAS particle-flow method that
combines charged-particle tracks and topo-clusters formed
from energy deposits in the calorimeter cells. The
anti-<jats:inline-formula><jats:alternatives><jats:tex-math>$$k_\textrm{t}$$</jats:tex-math>??
<mml:msub> <mml:mi>k</mml:mi> <mml:mtext>t</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
jet algorithm with radius parameter <jats:inline-formula><jats:alternatives><jats:tex-math>$$R=0.4$$</jats:tex-math>??
<mml:mrow> <mml:mi>R</mml:mi> <mml:mo>=</mml:mo>
<mml:mn>0.4</mml:mn> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula>
is used to define the jet. Novel jet energy scale
calibration strategies developed for the LHC Run 2 are
reported that lay the foundation for the jet calibration in
Run 3. Jets are calibrated with a series of simulation-based
corrections, including state-of-the-art techniques in jet
calibration such as machine learning methods and novel in
situ calibrations to achieve better performance than the
baseline calibration derived using up to 81
fb<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{-1}$$</jats:tex-math>??
<mml:msup> <mml:mrow /> <mml:mrow> <mml:mo>-</mml:mo>
<mml:mn>1</mml:mn> </mml:mrow> </mml:msup>
</mml:math></jats:alternatives></jats:inline-formula> of Run
2 data. The performance of these new techniques is then
examined in the in situ measurements by exploiting the
transverse momentum balance between a jet and a reference
object. The <jats:italic>b</jats:italic>-quark jet energy
scale using particle flow jets is measured for the first
time with around 1% precision using <jats:inline-formula><jats:alternatives><jats:tex-math>$$\gamma
$$</jats:tex-math>?? <mml:mi>γ</mml:mi>
</mml:math></jats:alternatives></jats:inline-formula>+jet
events.</jats:p>},
Doi = {10.1140/epjc/s10052-023-11837-9},
Key = {fds375911}
}
@article{fds308376,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Novel inclusive search for the Higgs boson in the
four-lepton final state at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {7},
Year = {2012},
Month = {October},
url = {http://inspirehep.net/record/1123369},
Abstract = {An inclusive search for the standard model Higgs boson using
the four-lepton final state in proton-antiproton collisions
produced by the Tevatron at √s=1.96TeV is conducted. The
data are recorded by the CDF II detector and correspond to
an integrated luminosity of 9.7fb -1. Three distinct Higgs
decay modes, namely ZZ, WW, and ττ, are simultaneously
probed. Nine potential signal events are selected and found
to be consistent with the background expectation. We set a
95% credibility limit on the production cross section times
the branching ratio and subsequent decay to the four-lepton
final state for hypothetical Higgs boson masses between
120GeV/c2 and 300GeV/c2. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.072012},
Key = {fds308376}
}
@article{fds308625,
Author = {Aaltonen, and T, and others},
Title = {Observation and mass measurement of the baryon
$Xi_b^-$},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {5},
Pages = {052002},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.052002},
Abstract = {We report the observation and measurement of the mass of the
bottom, strange baryon Xib- through the decay chain
Xib--->J/psiXi-, where J/psi-->µ+µ-, Xi--->Lambdapi-, and
Lambda-->ppi-. A signal is observed whose probability of
arising from a background fluctuation is 6.6{\AA}~10-15, or
7.7 Gaussian standard deviations. The Xib- mass is measured
to be 5792.9$\pm$2.5(stat) $\pm$1.7(syst)
MeV/c2.},
Doi = {10.1103/physrevlett.99.052002},
Key = {fds308625}
}
@article{fds321240,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Observation and measurement of Higgs boson decays to
WW∗with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.92.012006},
Abstract = {We report the observation of Higgs boson decays to
WW∗based on an excess over background of 6.1 standard
deviations in the dilepton final state, where the Standard
Model expectation is 5.8 standard deviations. Evidence for
the vector-boson fusion (VBF) production process is obtained
with a significance of 3.2 standard deviations. The results
are obtained from a data sample corresponding to an
integrated luminosity of 25 fb-1from √s = 7 and 8 TeV pp
collisions recorded by the ATLAS detector at the LHC. For a
Higgs boson mass of 125.36 GeV, the ratio of the measured
value to the expected value of the total production cross
section times branching fraction is 1.09+0.16-0.15(stat)+0.17-0.14(syst).
The corresponding ratios for the gluon fusion and
vector-boson fusion production mechanisms are 1.02 ±
0.19(stat)+0.22-0.18(syst) and 1.27+0.44-0.40(stat)+0.30-0.21(syst),
respectively. At √s = 8 TeV, the total production cross
sections are measured to be σ(gg→H→WW∗)=4.6±0.9(stat)+0.8-0.7(syst)
pb and σ(VBF H → WW∗)=0.51+0.17-0.15(stat)+0.13-0.08(syst)pb.
The fiducial cross section is determined for the
gluon-fusion process in exclusive final states with zero or
one associated jet.},
Doi = {10.1103/PhysRevD.92.012006},
Key = {fds321240}
}
@article{fds321294,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov,
SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell,
WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger,
N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G and Conventi, F and Cooke, M and Cooper,
BD},
Title = {Observation and measurements of the production of prompt and
non-prompt [Formula: see text] mesons in association with a
[Formula: see text] boson in [Formula: see text] collisions
at [Formula: see text] with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {5},
Pages = {229},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3406-9},
Abstract = {The production of a [Formula: see text] boson in association
with a [Formula: see text] meson in proton-proton collisions
probes the production mechanisms of quarkonium and heavy
flavour in association with vector bosons, and allows
studies of multiple parton scattering. Using [Formula: see
text] of data collected with the ATLAS experiment at the LHC
in [Formula: see text] collisions at [Formula: see text],
the first measurement of associated [Formula: see text]
production is presented for both prompt and non-prompt
[Formula: see text] production, with both signatures having
a significance in excess of [Formula: see text]. The
inclusive production cross-sections for [Formula: see text]
boson production (analysed in [Formula: see text] or
[Formula: see text] decay modes) in association with prompt
and non-prompt [Formula: see text] are measured relative to
the inclusive production rate of [Formula: see text] bosons
in the same fiducial volume to be [Formula: see text] and
[Formula: see text] respectively. Normalised differential
production cross-section ratios are also determined as a
function of the [Formula: see text] transverse momentum. The
fraction of signal events arising from single and double
parton scattering is estimated, and a lower limit of
[Formula: see text] at [Formula: see text] confidence level
is placed on the effective cross-section regulating double
parton interactions.},
Doi = {10.1140/epjc/s10052-015-3406-9},
Key = {fds321294}
}
@article{fds308655,
Author = {Abulencia, and A, and others},
Title = {Observation of $B^0_s \to K^{+} K^{-}$ and Measurements of
Branching Fractions of Charmless Two-body Decays of $B^0$
and $B^0_{s}$ Mesons in $\bar{p} p$ Collisions at $\sqrt{s}$
= 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {97},
Number = {21},
Pages = {211802},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.97.211802},
Abstract = {We search for decays of the type B(s)0-->h+h[prime]- (where
h,h[prime]=K or pi) in 180 pb-1 of [overline p]p collisions
collected at the Tevatron by the upgraded Collider Detector
at Fermilab. We report the first observation of the new mode
Bs0-->K+K- with a yield of 236$\pm$32 events, corresponding
to (fs/fd)?[script B](Bs0-->K+K-)/[script
B](B0-->K+pi-)=0.46$\pm$0.08(stat)$\pm$0.07(syst), where
fs/fd is the ratio of production fractions of Bs0 and B0. We
find results in agreement with world averages for the B0
modes, and set the following new limits at 90\% C.L.:
[script B](Bs0-->K-pi+)s0-->pi+pi-)},
Doi = {10.1103/physrevlett.97.211802},
Key = {fds308655}
}
@article{fds308628,
Author = {Abulencia, and A, and others},
Title = {Observation of $WZ$ Production},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {16},
Pages = {161801},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.161801},
Abstract = {We report the first observation of the associated production
of a W boson and a Z boson. This result is based on 1.1 fb-1
of integrated luminosity from p[overline p] collisions at
sqrt(s)=1.96 TeV collected with the CDF II detector at the
Fermilab Tevatron. We observe 16 WZ candidates passing our
event selection with an expected background of 2.7$\pm$0.4
events. A fit to the missing transverse energy distribution
indicates an excess of events compared to the background
expectation corresponding to a significance equivalent to 6
standard deviations. The measured cross section is
sigma(p[overline p]-->WZ)=5.0-1.6+1.8 pb, consistent with
the standard model expectation.},
Doi = {10.1103/physrevlett.98.161801},
Key = {fds308628}
}
@article{fds308452,
Author = {Aaltonen, and T, and al, E},
Title = {Observation of ${B}_{s}^{0}$\rightarrow${}J/$\psi${}{K}^{*}(892{)}^{0}$
and ${B}_{s}^{0}$\rightarrow${}J/$\psi${}{K}_{S}^{0}$
decays},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {5},
Pages = {052012},
Publisher = {American Physical Society},
Year = {2011},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.83.052012},
Abstract = {We report the first observation of two Cabibbo-suppressed
decay modes of the Bs0 meson. Using a sample of pp̄
collisions at √s=1.96TeV corresponding to 5.9fb-1 of
integrated luminosity collected with the CDF II, the
collider detector at the Fermilab Tevatron, we search for
new Bs0 decay modes in a sample of events containing
J/ψ→μ+μ - decays. We reconstruct a Bs0→J/ψK*(892)0
signal with K*(892)0→K+π-, observing a yield of 151±25
events with a statistical significance of 8.0σ. We also
reconstruct a Bs0→J/ψKS0 signal with KS0→π+π-,
observing a yield of 64±14 events with a statistical
significance of 7.2σ. From these yields, we extract the
branching ratios B(Bs0→J/ψK*(892)0)=(8. 3±3.8)×10-5 and
B(Bs0→J/ψK0)=(3.5±0.8) ×10-5, where statistical,
systematic, and fragmentation- fraction uncertainties are
included in the combined uncertainty. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevD.83.052012},
Key = {fds308452}
}
@article{fds375902,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez,
O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal,
D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour,
G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr,
AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano
Hurrell, LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir,
M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir,
O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone,
A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin,
E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F},
Title = {Observation of an Excess of Dicharmonium Events in the
Four-Muon Final State with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {15},
Pages = {151902},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.131.151902},
Abstract = {A search is made for potential ccc[over ¯]c[over ¯]
tetraquarks decaying into a pair of charmonium states in the
four muon final state using proton-proton collision data at
sqrt[s]=13 TeV, corresponding to an integrated
luminosity of 140 fb^{-1} recorded by the ATLAS
experiment at LHC. Two decay channels, J/ψ+J/ψ→4μ and
J/ψ+ψ(2S)→4μ, are studied. Backgrounds are estimated
based on a hybrid approach involving Monte Carlo
simulations and data-driven methods. Statistically
significant excesses with respect to backgrounds dominated
by the single parton scattering are seen in the di-J/ψ
channel consistent with a narrow resonance at 6.9 GeV and a
broader structure at lower mass. A statistically significant
excess is also seen in the J/ψ+ψ(2S) channel. The fitted
masses and decay widths of the structures are
reported.},
Doi = {10.1103/physrevlett.131.151902},
Key = {fds375902}
}
@article{fds321313,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin,
M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea,
V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov,
A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG},
Title = {Observation of an excited Bc(±) meson state with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {113},
Number = {21},
Pages = {212004},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.113.212004},
Abstract = {A search for excited states of the Bc(±) meson is performed
using 4.9 fb(-1) of 7 TeV and 19.2 fb(-1) of 8 TeV
pp collision data collected by the ATLAS experiment at the
LHC. A new state is observed through its hadronic transition
to the ground state, with the latter detected in the decay
Bc(±)→J/ψπ(±). The state appears in the
m(Bc(±)π(+)π(-))-m(Bc(±))-2m(π(±)) mass difference
distribution with a significance of 5.2 standard deviations.
The mass of the observed state is 6842±4±5 MeV, where
the first error is statistical and the second is systematic.
The mass and decay of this state are consistent with
expectations for the second S-wave state of the Bc(±)
meson, Bc(±)(2S).},
Doi = {10.1103/physrevlett.113.212004},
Key = {fds321313}
}
@article{fds308332,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu,
E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee,
P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behar Harpaz and S and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brown, G and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou,
Y},
Title = {Observation of associated near-side and away-side long-range
correlations in sqrt[s(NN)]=5.02 TeV proton-lead collisions
with the ATLAS detector.},
Journal = {Physical review letters},
Volume = {110},
Number = {18},
Pages = {182302},
Year = {2013},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.110.182302},
Abstract = {Two-particle correlations in relative azimuthal angle (Δø)
and pseudorapidity (Δη) are measured in sqrt[s(NN)] = 5.02
TeV p+Pb collisions using the ATLAS detector at the LHC. The
measurements are performed using approximately 1 μb(-1) of
data as a function of transverse momentum (p(T)) and the
transverse energy (ΣE(T)(Pb)) summed over 3.1 < η < 4.9 in
the direction of the Pb beam. The correlation function,
constructed from charged particles, exhibits a long-range (2
< |Δ η | < 5) "near-side" (Δø ~ 0) correlation that
grows rapidly with increasing ΣE(T)(Pb). A long-range
"away-side" (Δø ~ π) correlation, obtained by subtracting
the expected contributions from recoiling dijets and other
sources estimated using events with small ΣE(T)(Pb), is
found to match the near-side correlation in magnitude, shape
(in Δη and Δø) and ΣE(T)(Pb) dependence. The resultant
Δø correlation is approximately symmetric about π/2, and
is consistent with a dominant cos2Δø modulation for all
ΣE(T)(Pb) ranges and particle p(T).},
Doi = {10.1103/physrevlett.110.182302},
Key = {fds308332}
}
@article{fds348712,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carrillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copie, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas,
J and Culbertson, R and Cully, JC and Cyr, D and DaRonco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Ceceo,
SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and DiTuro,
P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin,
M and Freeman, JC and Frisch, HJ and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay,
C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson,
A and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths,
M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hare, K and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean,
R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martinez, M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez,
PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nagano, A and Naganoma, J and Nahn, S and Nakano, and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Porteil, X and Poukhov, O and Pounder, N and Prokoshin, F and Pronko, A and Proudfoot, J and Ptochos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ranjan,
N and Rappoccio, S and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
I},
Title = {Observation of B s0 - B̄
s0 oscillations},
Journal = {Physical Review Letters},
Volume = {97},
Number = {24},
Pages = {242003},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevLett.97.242003},
Abstract = {We report the observation of B s0- B̄ s0 oscillations from
a time-dependent measurement of the B s0-B̄ s0 oscillation
frequency Δm s. Using a data sample of 1 fb -1 of pp
collisions at √ = 1.96 TeV collected with the CDF II
detector at the Fermilab Tevatron, we find signals of 5600
fully reconstructed hadronic B s decays, 3100 partially
reconstructed hadronic B s decays, and 61500 partially
reconstructed semileptonic B s decays. We measure the
probability as a function of proper decay time that the B s
decays with the same, or opposite, flavor as the flavor at
production, and we find a signal for B s0-B̄ s0
oscillations. The probability that random fluctuations could
produce a comparable signal is 8 × 10 -8, which exceeds 5σ
significance. We measure Δm s = 17.77 ± 0.10(stat) ±
0.07(syst) ps -1 and extract |V td/V ts| = 0.2060 ±
0.0007(Δm s) -0.0060+0.0081 (Δm d + theor). © 2006 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.97.242003},
Key = {fds348712}
}
@article{fds308840,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Culbertson, R and Dagenhart, D and Daniels, T and Jongh, FD and dell'Agnello, S and dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and Compte, TL and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi,
E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukheņee, A and Muller, T and Murat, P and Murgia, S and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh,
SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips,
TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni,
A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt,
MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill,
A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok,
K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima,
R and Takikawa, K and Tanaka, M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko,
M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and Vejcik, S and Velev, G and Vidal, R and Vilar,
R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh,
GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Observation of Bc mesons in pp̄ collisions at
√s = 1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {58},
Number = {11},
Pages = {1120041+11200429},
Year = {1998},
Abstract = {We report the observation of bottom-charmed mesons Bc ni 1.8
TeV pp̄ collisions using the CDF detector at the Fermilab
Tevatron. The Bc mesons were found through their
semileptonic decays, B±c → J/ψl± X. A fit to the J/ψl
mass distribution yielded 20.4+6.2-5.5 events from Bc
mesons. A test of the null hypothesis, i.e., an attempt to
fit the data with background alone, was rejected at the
level of 4.8 standard deviations. By studying the quality of
the fit as a function of the assumed Bc mass, we determined
M(Bc) = 6.40 ±0.39 (stat.)±0.13 (syst) GeV/c2. From the
distribution of trilepton intersection points in the plane
transverse to the beam direction we measure the Bc lifetime
to be τ(Bc) = 0.46+0.18-0.16 (stat)±0.03 (syst) ps. We
also measured the ratio of production cross section times
branching fraction for B+c → J/ψl+ v relative to that for
B+ → J/ψK+ to be σ(Bc)×B(B c→J/ψlv)/σ(B)×B(B→J/ψK)
= 0.132+0.041-0.037 (stat)±0.031 (syst)+0.032-0.020(lifetime).},
Key = {fds308840}
}
@article{fds308841,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Culbertson, R and Dagenhart, D and Daniels, T and Jongh, FD and dell'Agnello, S and dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Nakano, I and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and Compte, TL and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer,
N and Long, O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Nakada, H and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg,
D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith,
C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella,
F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka, M and Tannenbaum,
B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto,
Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk,
W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal,
R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson,
R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Observation of B+ → ψ(2S)K+ and
B0 → ψ(2S)K*(892)0 decays and
measurements of B-meson branching fractions into J/ ψ and
ψ(2S) final states},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {58},
Number = {7},
Pages = {720011-720012+7200115},
Year = {1998},
ISSN = {0556-2821},
Abstract = {We report the observations of the decays B+ → ψ(2S)K+ and
B0 → ψ(2S)K*(892)0 in pp̄ collisions at a center-of-mass
energy of 1.8 TeV using a 110 pb-1 data sample recorded by
the Collider Detector at Fermilab. We also reconstruct the
decays B+ → J/ψK+ and B0 → J/ψK*(892)0 and measure the
six ratios of branching fractions of these four decays. The
relative branching-fraction results are shown to be
consistent with phenomenological factorization calculations
of hadronic B-meson decays. We use the world-average
branching fraction ℬ(B+ → J/ψK+) to derive ℬ(B+ →
ψ(2S)K+) = (0.56±0.08±0.10) × 10-3, ℬ(B0 →
ψ(2S)K*(892)0) = (0.92±0.20±0.16) × 10-3, and ℬ(B0 →
J/ψK*(892)0) = (1.78±0.14±0.29) × 10-3, where the first
and second uncertainties are statistical and systematic,
respectively.},
Key = {fds308841}
}
@article{fds344675,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo,
T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
I and Gallinaro, M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris,
N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and Gonzalez, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper,
S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer, A and Heinemann, B and Heinrich, J and Herndon, M and Hidas,
D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun,
SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato, Y and Kemp,
Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee,
YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister,
A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto,
A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
E and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava,
R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin,
A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton, P and Rescigno, M and Richter, S and Rimondi,
F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers,
E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz,
A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti,
A and Sinervo, P and Sisakyan, A and Sjolin, J},
Title = {Observation of Bs0→ψ(2S) and measurement of the ratio of
branching fractions B(Bs0→ψ(2S) /B(Bs0→J/ψ)},
Journal = {Physical Review Letters},
Volume = {96},
Number = {23},
Pages = {231801},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevLett.96.231801},
Abstract = {We report the first observation of Bs0→ψ(2S) decay in
pp̄ collisions at s= 1.96 TeV using 360 pb-1 of data
collected by the CDF II detector at the Fermilab Tevatron.
We observe 20.2±5.0 and 12.3±4.1 Bs0→ψ(2S) candidates,
in ψ(2S)→μ+μ- and ψ(2S)→J/ψπ+π- decay modes,
respectively. We present a measurement of the relative
branching fraction B(Bs0→ψ(2S) /B(Bs0→J/ψ)=0.52±0.13(stat)±0.04(syst)±0.06(BR)
using the ψ(2S)→μ+μ- decay mode. © 2006 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.96.231801},
Key = {fds344675}
}
@article{fds308784,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Borras, K and Bortoletto,
D and Boudreau, J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro,
A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Convery, ME and Conway, J and Cordelli, M and Cranshaw,
J and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Dominguez,
A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Erbacher, R and Errede, D and Errede, S and Fan, Q and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov,
I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian,
G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa,
T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Lee, AM and Lee, K and Leone, S and Lewis, JD and Lindgren,
M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Roy,
A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg,
D and Sanchez, C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding,
J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda,
H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
F and Vaiciulis, T and Valls, J and Vejcik, S and Velev, G and Veramendi,
G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters,
D and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Observation of diffractive J/ψ production at the Fermilab
Tevatron},
Journal = {Physical Review Letters},
Volume = {87},
Number = {24},
Pages = {2418021-2418026},
Year = {2001},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.87.241802},
Abstract = {The first observation of diffractive J/ψ(→μ+μ-)
production in p̄p collisions at s√=1.8 TeV was presented.
Events were selected with a pair of muon candidates using a
three-level dimuon trigger system. The dimuon mass
distribution was fitted with a sum of a Gaussian and a
linear function to evaluate the fraction of background
events in the signal region. A value of 0.59±0.15 for the
gluon fraction of the diffractive structure function of the
proton was extracted.},
Doi = {10.1103/physrevlett.87.241802},
Key = {fds308784}
}
@article{fds308867,
Author = {al, FAE},
Title = {Observation of diffractive W-boson production at the
Fermilab tevatron},
Journal = {Phys. Rev. Lett.},
Volume = {78},
Number = {14},
Pages = {2698-2703},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevLett.78.2698},
Abstract = {We report the first observation of diffractively produced W
bosons.In a sample of W → eν events produced in pp
collisions at √s=1.8TeV, we find an excess of events with
a forward rapidity gap, which is attributed to
diffraction.The probability that this excess is consistent
with nondiffractive production is 1.1×10−4 (3.8σ).The
relatively low fraction of W+ jet events observed within
this excess implies that mainly quarks from the Pomeron,
which mediates diffraction, participate in W production.The
diffractive to nondiffractive W production ratio is found to
be RW=(1.15±0.55)%.© 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.78.2698},
Key = {fds308867}
}
@article{fds308294,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kulkarni, N and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta,
A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra,
A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S},
Title = {Observation of D⁰-D¯⁰ mixing using the CDF II
detector.},
Journal = {Physical review letters},
Volume = {111},
Number = {23},
Pages = {231802},
Year = {2013},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.111.231802},
Abstract = {We measure the time dependence of the ratio of decay rates
for D0→K(+)π(-) to the Cabibbo-favored decay
D(0)→K(-)π(+). The charge conjugate decays are included.
A signal of 3.3×10(4) D(*+)→π(+)D(0), D(0)→K(+)π(-)
decays is obtained with D0 proper decay times between 0.75
and 10 mean D0 lifetimes. The data were recorded with the
CDF II detector at the Fermilab Tevatron and correspond to
an integrated luminosity of 9.6 fb(-1) for pp¯
collisions at √s=1.96 TeV. Assuming CP conservation,
we search for D0-D¯0 mixing and measure the mixing
parameters to be R(D)=(3.51±0.35)×10(-3),
y'=(4.3±4.3)×10(-3), and x'2=(0.08±0.18)×10(-3). We
report Bayesian probability intervals in the x'2-y' plane
and find that the significance of excluding the no-mixing
hypothesis is equivalent to 6.1 Gaussian standard
deviations, providing the second observation of D0-D¯0
mixing from a single experiment.},
Doi = {10.1103/physrevlett.111.231802},
Key = {fds308294}
}
@article{fds365361,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Observation of electroweak production of two jets in
association with an isolated photon and missing transverse
momentum, and search for a Higgs boson decaying into
invisible particles at 13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {2},
Year = {2022},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09878-z},
Abstract = {This paper presents a measurement of the electroweak
production of two jets in association with a Zγ pair, with
the Z boson decaying into two neutrinos. It also presents a
search for invisible or partially invisible decays of a
Higgs boson with a mass of 125 GeV produced through
vector-boson fusion with a photon in the final state. These
results use data from LHC proton–proton collisions at s =
13 TeV collected with the ATLAS detector and corresponding
to an integrated luminosity of 139 fb - 1. The event
signature, shared by all benchmark processes considered for
the measurements and searches, is characterized by a
significant amount of unbalanced transverse momentum and a
photon in the final state, in addition to a pair of forward
jets. Electroweak Zγ production in association with two
jets is observed in this final state with a significance of
5.2 (5.1 expected) standard deviations. The measured
fiducial cross-section for this process is 1.31 ± 0.29 fb.
An observed (expected) upper limit of 0.37 (0.34-0.10+0.15)
at 95% confidence level is set on the branching ratio of a
125 GeV Higgs boson to invisible particles, assuming the
Standard Model production cross-section. The signature is
also interpreted in the context of decays of a Higgs boson
into a photon and a dark photon. An observed (expected) 95%
CL upper limit on the branching ratio for this decay is set
at 0.018 (0.017-0.005+0.007), assuming the Standard Model
production cross-section for a 125 GeV Higgs
boson.},
Doi = {10.1140/epjc/s10052-021-09878-z},
Key = {fds365361}
}
@article{fds308519,
Author = {Aaltonen, T and others},
Title = {Observation of Electroweak Single Top-Quark
Production},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {9},
Pages = {092002},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.092002},
Abstract = {We report the observation of single top-quark production
using 3.2 fb-1 of pp̅ collision data with
sqrt[s]=1.96 TeV collected by the Collider Detector at
Fermilab. The significance of the observed data is 5.0
standard deviations, and the expected sensitivity for
standard model production and decay is in excess of 5.9
standard deviations. Assuming mt=175 GeV/c2, we measure
a cross section of 2.3-0.5+0.6(stat+syst) pb, extract
the CKM matrix-element value |Vtb|=0.91 ±
0.11(stat+syst) ± 0.07(theory), and set the limit
|Vtb|>0.71 at the 95% C.L.},
Doi = {10.1103/physrevlett.103.092002},
Key = {fds308519}
}
@article{fds308542,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey,
P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani,
M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Hamilton, A and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko,
BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal,
AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan,
P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla
Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla,
A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer,
B},
Title = {Observation of exclusive charmonium production and
gammagamma --> micro;{+}micro;{-} in pp[over] collisions at
sqrt[s] = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {102},
Number = {24},
Pages = {242001},
Year = {2009},
Month = {June},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.102.242001},
Abstract = {In CDF we have observed the reactions p + p[over] --> p + X
+ p[over], with X being a centrally produced J/psi, psi(2S),
or chi_{c0}, and gammagamma-->micro;{+}micro;{-} in pp[over]
collisions at sqrt[s] = 1.96 TeV. The event signature
requires two oppositely charged central muons, and either no
other particles or one additional photon detected. Exclusive
vector meson production is as expected for elastic
photoproduction, gamma + p --> J/psi(psi(2S)) + p, observed
here for the first time in hadron-hadron collisions. We also
observe exclusive chi_{c0} --> J/psi + gamma. The cross
sections dsigma/dy|_{y = 0} for J/psi, psi(2S), and chi_{c0}
are 3.92 +/- 0.25(stat) +/- 0.52(syst) nb, 0.53 +/-
0.09(stat) +/- 0.10(syst) nb, and 76 +/- 10(stat) +/-
10(syst) nb, respectively, and the continuum is consistent
with QED. We put an upper limit on the cross section for
Odderon exchange in exclusive J/psi production.},
Doi = {10.1103/physrevlett.102.242001},
Key = {fds308542}
}
@article{fds308394,
Author = {Aaltonen, T and others},
Title = {Observation of Exclusive Charmonium Production and
γγ→μ+μ- in pp̅ Collisions at sqrt[s] =1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {24},
Pages = {242001},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.108.081801},
Abstract = {In CDF we have observed the reactions p+p̅ →p+X+p̅ ,
with X being a centrally produced J/ψ, ψ(2S), or χc0, and
γγ→μ+μ- in pp̅ collisions at sqrt[s]=1.96 TeV.
The event signature requires two oppositely charged central
muons, and either no other particles or one additional
photon detected. Exclusive vector meson production is as
expected for elastic photoproduction, γ+p→J/ψ(ψ(2S))+p,
observed here for the first time in hadron-hadron
collisions. We also observe exclusive χc0→J/ψ+γ. The
cross sections dσ / dy|y=0 for J/ψ, ψ(2S), and χc0 are
3.92 ± 0.25(stat) ± 0.52(syst) nb, 0.53
± 0.09(stat) ± 0.10(syst) nb, and 76
± 10(stat) ± 10(syst) nb, respectively,
and the continuum is consistent with QED. We put an upper
limit on the cross section for Odderon exchange in exclusive
J/ψ production.},
Doi = {10.1103/physrevlett.108.081801},
Key = {fds308394}
}
@article{fds308632,
Author = {Abulencia, and A, and others},
Title = {Observation of exclusive electron positron production in
hadron hadron collisions},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {11},
Pages = {112001},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.112001},
Abstract = {We present the first observation of exclusive e+e-
production in hadron-hadron collisions, using p[overline p]
collision data at sqrt(s)=1.96 TeV taken by the run II
Collider Detector at Fermilab, and corresponding to an
integrated luminosity of 532 pb-1. We require the absence of
any particle signatures in the detector except for an
electron and a positron candidate, each with transverse
energy ET>5 GeV and pseudorapidity |eta|p+e+e-+[overline p]
through two-photon exchange. The measured cross section is
1.6-0.3+0.5(stat)$\pm$0.3(syst) pb. This agrees with the
theoretical prediction of 1.71$\pm$0.01 pb.},
Doi = {10.1103/physrevlett.98.112001},
Key = {fds308632}
}
@article{fds375946,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Cardoso, MA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler,
A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA},
Title = {Observation of four-top-quark production in the multilepton
final state with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11573-0},
Abstract = {This paper presents the observation of four-top-quark (tt¯
tt¯) production in proton-proton collisions at the LHC. The
analysis is performed using an integrated luminosity of 140
fb - 1 at a centre-of-mass energy of 13 TeV collected using
the ATLAS detector. Events containing two leptons with the
same electric charge or at least three leptons (electrons or
muons) are selected. Event kinematics are used to separate
signal from background through a multivariate discriminant,
and dedicated control regions are used to constrain the
dominant backgrounds. The observed (expected) significance
of the measured tt¯ tt¯ signal with respect to the
standard model (SM) background-only hypothesis is 6.1 (4.3)
standard deviations. The tt¯ tt¯ production cross section
is measured to be 22.5-5.5+6.6 fb, consistent with the SM
prediction of 12.0 ± 2.4 fb within 1.8 standard deviations.
Data are also used to set limits on the three-top-quark
production cross section, being an irreducible background
not measured previously, and to constrain the top-Higgs
Yukawa coupling and effective field theory operator
coefficients that affect tt¯ tt¯ production.},
Doi = {10.1140/epjc/s10052-023-11573-0},
Key = {fds375946}
}
@article{fds375912,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V},
Title = {Observation of gauge boson joint-polarisation states in
W±Z production from pp collisions at s=13 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137895},
Abstract = {Measurements of joint-polarisation states of W and Z gauge
bosons in W±Z production are presented. The data set used
corresponds to an integrated luminosity of 139 fb−1 of
proton–proton collisions at a centre-of-mass energy of 13
TeV recorded by the ATLAS detector at the CERN Large Hadron
Collider. The W±Z candidate events are reconstructed using
leptonic decay modes of the gauge bosons into electrons and
muons. The simultaneous pair-production of longitudinally
polarised vector bosons is measured for the first time with
a significance of 7.1 standard deviations. The measured
joint helicity fractions integrated over the fiducial region
are f00=0.067±0.010, f0T=0.110±0.029, fT0=0.179±0.023 and
fTT=0.644±0.032, in agreement with the next-to-leading-order
Standard Model predictions. Individual helicity fractions of
the W and Z bosons are also measured and found to be
consistent with joint helicity fractions within the expected
amounts of correlation. Both the joint and individual
helicity fractions are also measured separately in W+Z and
W−Z events. Inclusive and differential cross sections for
several kinematic observables sensitive to polarisation are
presented.},
Doi = {10.1016/j.physletb.2023.137895},
Key = {fds375912}
}
@article{fds330942,
Author = {Collaboration, CDF},
Title = {Observation of Hadronic W Decays in tt Events with the
Collider Detector at Fermilab},
Journal = {Phys. Rev. Lett.},
Volume = {80},
Number = {26},
Pages = {5720},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.5720},
Abstract = {We observe hadronic W decays in tt →W(→ lv)+≥4 jet
events using a 109 pb data sample of pp collisions at
s=1.8TeV collected with the Collider Detector at Fermilab. A
peak in the dijet invariant mass distribution is obtained
that is consistent with W decay and inconsistent with the
background prediction by 3.3 σ.From this peak we measure
the W mass to be 77.2±4.6(stat+syst)GeV/c . This result
demonstrates the presence of a second W boson in tt
candidates in the W(→ lv)+≥jet channel. © 1998 American
Physical Society. ¯ −1 ¯ 2 ¯},
Doi = {10.1103/PhysRevLett.80.5720},
Key = {fds330942}
}
@article{fds316861,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo,
T},
Title = {Observation of Long-Range Elliptic Azimuthal Anisotropies in
sqrt[s]=13 and 2.76 TeV pp Collisions with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {116},
Number = {17},
Pages = {172301},
Year = {2016},
Month = {April},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.116.172301},
Abstract = {ATLAS has measured two-particle correlations as a function
of the relative azimuthal angle, Δϕ, and pseudorapidity,
Δη, in sqrt[s]=13 and 2.76 TeV pp collisions at the LHC
using charged particles measured in the pseudorapidity
interval |η|<2.5. The correlation functions evaluated in
different intervals of measured charged-particle
multiplicity show a multiplicity-dependent enhancement at
Δϕ∼0 that extends over a wide range of Δη, which has
been referred to as the "ridge." Per-trigger-particle
yields, Y(Δϕ), are measured over 2<|Δη|<5. For both
collision energies, the Y(Δϕ) distribution in all
multiplicity intervals is found to be consistent with a
linear combination of the per-trigger-particle yields
measured in collisions with less than 20 reconstructed
tracks, and a constant combinatoric contribution modulated
by cos(2Δϕ). The fitted Fourier coefficient, v_{2,2},
exhibits factorization, suggesting that the ridge results
from per-event cos(2ϕ) modulation of the single-particle
distribution with Fourier coefficients v_{2}. The v_{2}
values are presented as a function of multiplicity and
transverse momentum. They are found to be approximately
constant as a function of multiplicity and to have a p_{T}
dependence similar to that measured in p+Pb and Pb+Pb
collisions. The v_{2} values in the 13 and 2.76 TeV data
are consistent within uncertainties. These results suggest
that the ridge in pp collisions arises from the same or
similar underlying physics as observed in p+Pb collisions,
and that the dynamics responsible for the ridge has no
strong sqrt[s] dependence.},
Doi = {10.1103/physrevlett.116.172301},
Key = {fds316861}
}
@article{fds308522,
Author = {Aaltonen, T and others},
Title = {Observation of New Charmless Decays of Bottom
Hadrons},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {3},
Pages = {031801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.031801},
Abstract = {We search for new charmless decays of neutral b hadrons to
pairs of charged hadrons, using 1 fb-1 of data
collected by the CDF II detector at the Fermilab Tevatron.
We report the first observation of the Bs0→K-π+ decay and
measure B(Bs0→K-π+)=(5.0 ± 0.7(stat) ±
0.8(syst))×10-6. We also report the first observation of
charmless b-baryon decays, and measure B(Λb0→pπ-)=(3.5
± 0.6(stat) ± 0.9(syst))×10-6 and
B(Λb0→pK-)=(5.6 ± 0.8(stat) ±
1.5(syst))×10-6. No evidence is found for other modes, and
we set the limit B(Bs0→π+π-)<1.2×10-6 at 90%
C.L.},
Doi = {10.1103/physrevlett.103.031801},
Key = {fds308522}
}
@article{fds308267,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de Barbaro, P and de Jong, SJ and De La
Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov, SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto, F and Di Canto and A and Di Ruzza,
B and Diehl, HT and Diesburg, M and Ding, PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti,
A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, VN and Farrington, S and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov,
V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Grinstein, S and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De
La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere,
A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung,
AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim,
YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich, I and Knoepfel,
K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr,
T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster, M and Lannon,
K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li,
H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour,
J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega,
J and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta,
A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed,
S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett,
J and Neu, C and Neustroev, P},
Title = {Observation of s-channel production of single top quarks at
the Tevatron.},
Journal = {Physical review letters},
Volume = {112},
Number = {23},
Pages = {231803},
Year = {2014},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.112.231803},
Abstract = {We report the first observation of single-top-quark
production in the s channel through the combination of the
CDF and D0 measurements of the cross section in
proton-antiproton collisions at a center-of-mass energy of
1.96 TeV. The data correspond to total integrated
luminosities of up to 9.7 fb(-1) per experiment. The
measured cross section is σ(s) = 1.29(-0.24)(+0.26) pb. The
probability of observing a statistical fluctuation of the
background to a cross section of the observed size or larger
is 1.8 × 10(-10), corresponding to a significance of 6.3
standard deviations for the presence of an s-channel
contribution to the production of single-top
quarks.},
Doi = {10.1103/physrevlett.112.231803},
Key = {fds308267}
}
@article{fds308495,
Author = {Aaltonen, and T, and others},
Title = {Observation of single top quark production and measurement
of |$V_{tb}|$ with CDF},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {11},
Pages = {112005},
Publisher = {American Physical Society},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.82.112005},
Abstract = {We report the observation of electroweak single top quark
production in 3.2fb⊃-1 of pp̄ collision data collected by
the Collider Detector at Fermilab at √s=1.96TeV. Candidate
events in the W+jets topology with a leptonically decaying W
boson are classified as signal-like by four parallel
analyses based on likelihood functions, matrix elements,
neural networks, and boosted decision trees. These results
are combined using a super discriminant analysis based on
genetically evolved neural networks in order to improve the
sensitivity. This combined result is further combined with
that of a search for a single top quark signal in an
orthogonal sample of events with missing transverse energy
plus jets and no charged lepton. We observe a signal
consistent with the standard model prediction but
inconsistent with the background-only model by 5.0 standard
deviations, with a median expected sensitivity in excess of
5.9 standard deviations. We measure a production cross
section of 2.3-0.5+0.6(stat+sys)pb, extract the value of the
Cabibbo-Kobayashi-Maskawa matrix element |Vtb|=0.91-0.11+0.
11(stat+sys)±0.07(theory), and set a lower limit |Vtb|>0.71
at the 95%C.L., assuming mt=175GeV/c2.},
Doi = {10.1103/PhysRevD.82.112005},
Key = {fds308495}
}
@article{fds375898,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira,
MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos,
P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat,
A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley,
JR and Batool, B and Battaglia, M and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer,
JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi,
G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya,
DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
O and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov,
VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden
Madden, WD and Brendlinger, K and Brener, R and Brenner, L and Brenner,
R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de
Renstrom, PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov,
O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo
Garcia, L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi,
E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov,
MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A and Clark, PJ and Clavijo Columbie and JM and Clawson,
SE},
Title = {Observation of Single-Top-Quark Production in Association
with a Photon Using the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {18},
Pages = {181901},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.131.181901},
Abstract = {This Letter reports the observation of single top quarks
produced together with a photon, which directly probes the
electroweak coupling of the top quark. The analysis uses
139 fb^{-1} of 13 TeV proton-proton collision data
collected with the ATLAS detector at the Large Hadron
Collider. Requiring a photon with transverse momentum larger
than 20 GeV and within the detector acceptance, the
fiducial cross section is measured to be
688±23(stat) _{-71}^{+75}(syst) fb, to be compared
with the standard model prediction of 515_{-42}^{+36} fb
at next-to-leading order in QCD.},
Doi = {10.1103/physrevlett.131.181901},
Key = {fds375898}
}
@article{fds308430,
Author = {Aaltonen, and T, and al, E},
Title = {Observation of the $\Xi_{b}^{0}$ Baryon},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {10},
Pages = {102001},
Publisher = {American Physical Society},
Year = {2011},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.102001},
Abstract = {The observation of the bottom, strange baryon Ξ(b)(0)
through the decay chain Ξ(b)(0)→Ξ(c)(+)π-, where
ΞΞ(c)(+)→Ξ- π+ π+, Ξ-→Λπ-, and Λ→pπ-, is
reported by using data corresponding to an integrated
luminosity of 4.2 fb(-1) from pp collisions at square
root(s)=1.96 TeV recorded with the Collider Detector at
Fermilab. A signal of 25.3(-5.4)(+5.6) candidates is
observed whose probability of arising from a background
fluctuation is 3.6×10(-12), corresponding to 6.8 gaussian
standard deviations. The Ξ(b)(0) mass is measured to be
5787.8±5.0(stat)±1.3(syst) MeV/c2. In addition, the
Ξ(b)- baryon is observed through the process
Ξ(b)-→Ξ(c)(0)π-, where Ξ(c)(0)→Ξ- π+, Ξ-→Λπ-,
and Λ→pπ-.},
Doi = {10.1103/PhysRevLett.107.102001},
Key = {fds308430}
}
@article{fds308426,
Author = {Aaltonen, TEA},
Title = {Observation of the Baryonic Flavor-Changing Neutral Current
Decay $\Lambda_{b}^{0}\rightarrow\Lambda\mu^{+}\mu^{-}$},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {20},
Pages = {201802},
Publisher = {American Physical Society},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.201802},
Abstract = {We report the first observation of the baryonic
flavor-changing neutral current decay Λ(b)(0)→Λμ(+)μ(-)
with 24 signal events and a statistical significance of 5.8
Gaussian standard deviations. This measurement uses a pp
collisions data sample corresponding to 6.8 fb(-1) at √s =
1.96 TeV collected by the CDF II detector at the Tevatron
collider. The total and differential branching ratios for
Λ(b)(0)→Λμ(+)μ(-) are measured. We find
B(Λ(b)(0)→Λμ(+)μ(-))=[1.73 ± 0.42(stat) ± (syst)] ×
10(-6). We also report the first measurement of the
differential branching ratio of B(s)(0)→ϕμ(+)μ(-),
using 49 signal events. In addition, we report branching
ratios for B(+)→K(+)μ(+)μ(-), B(0)→K(0)μ(+)μ(-), and
B→K(*)(892)μ(+)μ(-) decays.},
Doi = {10.1103/PhysRevLett.107.201802},
Key = {fds308426}
}
@article{fds308834,
Author = {Collaboration, CDF},
Title = {Observation of the Bc Meson in pp Collisions at „© s =
1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {81},
Number = {12},
Pages = {2432},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.2432},
Abstract = {We have observed bottom-charm mesons via the decay mode B±c
→ J/ψl±ν in 1.8 TeV pp¯ collisions using the CDF
detector at the Fermilab Tevatron. A fit of background and
signal contributions to the J/ψl mass distribution yielded
20.4+6.2-5.5 events from Bc mesons. A fit to the same
distribution with background alone was rejected at the level
of 4.8 standard deviations. We measured the B+c mass to be
6.40 ± 0.39(stat) ± 0.13(syst) GeV/c2 and the B+c lifetime
to be 0.46+0.18-0.16(stat) ± 0.03(syst)ps. Our measured
yield (production cross section times branching ratio) for
B±c → J/ψl+ν relative to that for B+ → J/ψK+ is
0.132+0.041-0.037(stat) ± 0.031(syst)+0.032-0.020(lifetime).
© 1998 The American Physical Society.},
Doi = {10.1103/PhysRevLett.81.2432},
Key = {fds308834}
}
@article{fds361695,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Lorenzo,
GD and Dell'Orso, M and Demortier, L and Deng, J and Deninno, M and Pedis,
DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare,
M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun,
SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato,
Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson,
B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus, J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone,
S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, RS and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli,
F and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Griso,
SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic,
V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó,
O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ},
Title = {Observation of the decay Bc±→J/ψπ± and measurement of
the Bc± mass},
Journal = {Physical Review Letters},
Volume = {100},
Number = {18},
Pages = {182002},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevLett.100.182002},
Abstract = {The Bc± meson is observed through the decay Bc±→J/
ψπ±, in data corresponding to an integrated luminosity of
2.4fb-1 recorded by the Collider Detector at Fermilab II
detector at the Fermilab Tevatron. A signal of 108±15
candidates is observed, with a significance that exceeds
8σ. The mass of the Bc± meson is measured to be
6275.6±2.9(stat)±2.5(syst)MeV/c2. © 2008 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.100.182002},
Key = {fds361695}
}
@article{fds308637,
Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Behari,
S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and DaRonco, S and Datta, M and D'Auria, S and Davies, T and Dagenhart, D and de Barbaro, P and De
Cecco, S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'Orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Dörr,
C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron,
J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani,
M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson,
C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl,
D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marginean,
R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel,
P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles,
J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher,
G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore,
R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou,
A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov,
A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar,
S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
M and Shochet, M and Shon, Y},
Title = {Observation of the Heavy Baryons Sigma b and Sigma
b*.},
Journal = {Physical review letters},
Volume = {99},
Number = {20},
Pages = {202001},
Year = {2007},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.99.202001},
Abstract = {We report an observation of new bottom baryons produced in
pp collisions at the Tevatron. Using 1.1 fb(-1) of data
collected by the CDF II detector, we observe four Lambda b 0
pi+/- resonances in the fully reconstructed decay mode
Lambda b 0-->Lambda c + pi-, where Lambda c+-->pK* pi+. We
interpret these states as the Sigma b(*)+/- baryons and
measure the following masses: m Sigma b+=5807.8 -2.2
+2.0(stat.)+/-1.7(syst.) MeV/c2, m Sigma b-
=5815.2+/-1.0(stat.)+/-1.7(syst.) MeV/c2, and m(Sigma
b*)-m(Sigma b)=21.2-1.9 +2.0(stat.)-0.3+0.4(syst.)
MeV/c2.},
Doi = {10.1103/physrevlett.99.202001},
Key = {fds308637}
}
@article{fds308735,
Author = {Acosta, D and Affolder, T and Ahn, MH and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and Barbaro-Galtieri, A and Barker, G and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini,
G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov,
S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett,
K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura,
P and Campanelli, M and Campbell, M and Canepa, A and Carlsmith, D and Carron, S and Carosi, R and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen,
C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chu, ML and Chung, JY and Chung,
WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, MN and Connolly, A and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cranshaw, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and DaRonco, S and D'Auria, S and Barbaro, PD and Cecco,
SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers,
S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and Doksus, P and Dominguez, A and Donati,
S and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Frisch, H and Fujii, Y and Furic, I and Gaijar, A and Gallas, A and Gallinaro, M and Galyardt, J and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, DW and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hall, C and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke,
M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman,
KD and Holloway, A and Hou, S and Houlden, MA and Huang, Y and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
H and Jones, M and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim,
TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov,
K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer,
A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis,
JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loken, J and Loreti,
M and Loverre, P and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, A and Martin, M and Martin, V and Martinez, M and Maruyama, T and Matsunaga, H and Mattson,
M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Menzemer, S and Menzione, A and Merkel,
P and Mesropian, C and Messina, A and Meyer, A and Miao, T and Miladinovic,
N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mishina, M and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Moore, R and Morello, M and Moulik, T and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Oesterberg, K and Ogawa, T and Oh, S and Oh, YD and Ohsugi, T and Oishi, R and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari,
F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
H and Reichold, A and Rekovic, V and Renton, P and Rescigno, M and Rimondi,
F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni,
A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro,
A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shon, Y and Sidoti, A and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Somalwar, SV and Spalding, J and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Squillacioti, P and Stadie, H and Stelzer, B and Stelzer-Chilton, O and Strologas, J and Stuart, D and Sukhanov, A and Sumorok,
K},
Title = {Observation of the narrow state X(3872) →
J/ψπ+π- in p̄p collisions at √s
= 1.96 TeV},
Journal = {Physical Review Letters},
Volume = {93},
Number = {7},
Pages = {072001-1-072001-6},
Year = {2004},
url = {http://dx.doi.org/10.1103/PhysRevLett.93.072001},
Abstract = {The observation of a state consistent with X(3872) decaying
into J/ψπ+π- was reported. The X(3872) mass was measured
to be 3871.3±0.7(stat)±0.4(syst)MeV/c2 from a sample of
730±90 candidates. The observed width was consistent with
the detector resolution. The results were found to be
converging well with the measurements by the Belle
Collaboration using b± decays.},
Doi = {10.1103/PhysRevLett.93.072001},
Key = {fds308735}
}
@article{fds308351,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chou, JP and Chokheli,
D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza,
B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Funakoshi, Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hopkins, W and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leone, S and Lewis, JD and Limosani, A and Lipeles,
E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys,
J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty,
R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki,
D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore,
R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro,
A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi,
G and Wagner, P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams,
HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers,
S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato,
D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Observation of the production of a W boson in association
with a single charm quark.},
Journal = {Physical review letters},
Volume = {110},
Number = {7},
Pages = {071801},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.110.071801},
Abstract = {The first observation of the production of a W boson with a
single charm quark (c) jet in pp[over ¯] collisions at
√s=1.96 TeV is reported. The analysis uses data
corresponding to 4.3 fb(-1), recorded with the CDF II
detector at the Fermilab Tevatron. Charm quark candidates
are selected through the identification of an electron or
muon from charm-hadron semileptonic decay within a hadronic
jet, and a Wc signal is observed with a significance of 5.7
standard deviations. The production cross section
σ(Wc)(p(Tc)>20 GeV/c,|η(c)|<1.5)×B(W→ℓν) is
measured to be 13.6(-3.1)(+3.4) pb and is in agreement
with theoretical expectations. From this result the
magnitude of the quark-mixing matrix element V(cs) is
derived, |V(cs)|=1.08±0.16 along with a lower limit of
|V(cs)|>0.71 at the 95% confidence level, assuming that the
Wc production through c to s quark coupling is
dominant.},
Doi = {10.1103/physrevlett.110.071801},
Key = {fds308351}
}
@article{fds375903,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baron
Moreno, DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram,
IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Bisceglie,
E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden
Madden, WD and Brendlinger, K and Brener, R and Brenner, L and Brenner,
R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de
Renstrom, PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov,
O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo
Garcia, L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi,
E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro,
V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ and Clavijo
Columbie, JM},
Title = {Observation of the γγ→ττ Process in Pb+Pb Collisions
and Constraints on the τ-Lepton Anomalous Magnetic Moment
with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {15},
Pages = {151802},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.131.151802},
Abstract = {This Letter reports the observation of τ-lepton-pair
production in ultraperipheral lead-lead collisions
Pb+Pb→Pb(γγ→ττ)Pb and constraints on the τ-lepton
anomalous magnetic moment a_{τ}. The dataset corresponds to
an integrated luminosity of 1.44 nb^{-1} of LHC Pb+Pb
collisions at sqrt[s_{NN}]=5.02 TeV recorded by the
ATLAS experiment in 2018. Selected events contain one muon
from a τ-lepton decay, an electron or charged-particle
track(s) from the other τ-lepton decay, little additional
central-detector activity, and no forward neutrons. The
γγ→ττ process is observed in Pb+Pb collisions with a
significance exceeding 5 standard deviations and a signal
strength of μ_{ττ}=1.03_{-0.05}^{+0.06} assuming the
standard model value for a_{τ}. To measure a_{τ}, a
template fit to the muon transverse-momentum distribution
from τ-lepton candidates is performed, using a dimuon
(γγ→μμ) control sample to constrain systematic
uncertainties. The observed 95% confidence-level interval
for a_{τ} is -0.057<a_{τ}<0.024.},
Doi = {10.1103/physrevlett.131.151802},
Key = {fds375903}
}
@article{fds308561,
Author = {Aaltonen, T and others},
Title = {Observation of the Ωb- baryon and measurement of the
properties of the Ξb- and Ωb- baryons},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {7},
Pages = {072003},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.072003},
Abstract = {We report the observation of the bottom, doubly-strange
baryon Ωb- through the decay chain Ωb-→J/ψΩ-, where
J/ψ→μ+μ-, Ω-→ΛK-, and Λ→pπ-, using
4.2 fb-1 of data from pp̅ collisions at
sqrt[s]=1.96 TeV, and recorded with the Collider
Detector at Fermilab. A signal is observed whose probability
of arising from a background fluctuation is 4.0×10-8, or
5.5 Gaussian standard deviations. The Ωb- mass is measured
to be 6054.4 ± 6.8(stat) ±
0.9(syst) MeV/c2. The lifetime of the Ωb- baryon is
measured to be 1.13-0.40+0.53(stat) ±
0.02(syst) ps. In addition, for the Ξb- baryon we
measure a mass of 5790.9 ± 2.6(stat) ±
0.8(syst) MeV/c2 and a lifetime of 1.56-0.25+0.27(stat)
± 0.02(syst) ps. Under the assumption that the
Ξb- and Ωb- are produced with similar kinematic
distributions to the Λb0 baryon, we find
σ(Ξb-)B(Ξb-→J/ψΞ-) / σ(Λb0)B(Λb0→J/ψΛ)=0.167-0.025+0.037(stat)
± 0.012(syst) and σ(Ωb-)B(Ωb-→J/ψΩ-) /
σ(Λb0)B(Λb0→J/ψΛ)=0.045-0.012+0.017(stat) ±
0.004(syst) for baryons produced with transverse momentum in
the range of 6--20 GeV/c.},
Doi = {10.1103/PhysRevD.80.072003},
Key = {fds308561}
}
@article{fds321261,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Observation of top-quark pair production in association with
a photon and measurement of the t t ¯ γ production cross
section in pp collisions at √s =7 TeV using the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.91.072007},
Abstract = {A search is performed for top-quark pairs (tt¯) produced
together with a photon (γ) with transverse energy greater
than 20 GeV using a sample of tt¯ candidate events in final
states with jets, missing transverse momentum, and one
isolated electron or muon. The data set used corresponds to
an integrated luminosity of 4.59 fb-1 of proton-proton
collisions at a center-of-mass energy of 7 TeV recorded by
the ATLAS detector at the CERN Large Hadron Collider. In
total, 140 and 222 tt¯γ candidate events are observed in
the electron and muon channels, to be compared to the
expectation of 79±26 and 120±39 non-tt¯γ background
events, respectively. The production of tt¯γ events is
observed with a significance of 5.3 standard deviations away
from the null hypothesis. The tt¯γ production cross
section times the branching ratio (BR) of the single-lepton
decay channel is measured in a fiducial kinematic region
within the ATLAS acceptance. The measured value is
σtt¯γfid×BR=63±8(stat)-13+17(syst)±1(lumi) fb per
lepton flavor, in good agreement with the leading-order
theoretical calculation normalized to the
next-to-leading-order theoretical prediction of 48±10
fb.},
Doi = {10.1103/PhysRevD.91.072007},
Key = {fds321261}
}
@article{fds308889,
Author = {al, FAE},
Title = {Observation of top-quark production in (p)over-bar-p
collisions with the collider detector at
fermilab},
Journal = {Phys. Rev. Lett.},
Volume = {74},
Number = {14},
Pages = {2626-2631},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevLett.74.2626},
Abstract = {We establish the existence of the top quark using a 67 pb-1
data sample of p̄p collisions at s=1.8 TeV collected with
the Collider Detector at Fermilab (CDF). Employing
techniques similar to those we previously published, we
observe a signal consistent with tt̄ decay to WWbb̄, but
inconsistent with the background prediction by 4.8σ.
Additional evidence for the top quark is provided by a peak
in the reconstructed mass distribution. We measure the top
quark mass to be 176±8(stat)±10(syst) GeV/c2, and the tt̄
production cross section to be 6.8-2.4+3.6 pb. © 1995 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.74.2626},
Key = {fds308889}
}
@article{fds375882,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour,
G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr,
AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano
Hurrell, LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir,
M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir,
O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone,
A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin,
E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A},
Title = {Observation of WZγ Production in pp Collisions at
sqrt[s]=13 TeV with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {132},
Number = {2},
Pages = {021802},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.132.021802},
Abstract = {This Letter reports the observation of WZγ production and a
measurement of its cross section using 140.1±1.2 fb^{-1}
of proton-proton collision data recorded at a center-of-mass
energy of 13 TeV by the ATLAS detector at the Large Hadron
Collider. The WZγ production cross section, with both the W
and Z bosons decaying leptonically, pp→WZγ→ℓ^{'}^{±}νℓ^{+}ℓ^{-}γ
(ℓ^{(^{'})}=e, μ), is measured in a fiducial phase-space
region defined such that the leptons and the photon have
high transverse momentum and the photon is isolated. The
cross section is found to be 2.01±0.30(stat)±0.16(syst) fb.
The corresponding standard model predicted cross section
calculated at next-to-leading order in perturbative quantum
chromodynamics and at leading order in the electroweak
coupling constant is 1.50±0.06 fb. The observed
significance of the WZγ signal is 6.3σ, compared with an
expected significance of 5.0σ.},
Doi = {10.1103/physrevlett.132.021802},
Key = {fds375882}
}
@article{fds375988,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Observation of Wγγ triboson production in proton-proton
collisions at s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {848},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138400},
Abstract = {This letter reports the observation of W(ℓν)γγ
production in proton-proton collisions. This measurement
uses the full Run 2 sample of events recorded at a
center-of-mass energy of s=13 TeV by the ATLAS detector at
the LHC, corresponding to an integrated luminosity of 140
fb−1. Events with a leptonically-decaying W boson and at
least two photons are considered. The background-only
hypothesis is rejected with an observed and expected
significance of 5.6 standard deviations. The inclusive
fiducial production cross section of W(eν)γγ and
W(μν)γγ events is measured to be σfid=13.8±1.1(stat)+2.1−2.0(syst)±0.1(lumi)
fb, in agreement with the Standard Model
prediction.},
Doi = {10.1016/j.physletb.2023.138400},
Key = {fds375988}
}
@article{fds308851,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg,
C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane,
D and Cronin-Hennessy, D and Culbertson, R and Daniels, T and DeJongh,
F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Dunn, A and Eddy,
N and Einsweiler, K and Elias, JE and Ely, R and Engels, E and Errede, D and Errede, S and Fan, Q and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman,
J and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti,
S and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gladney, L and Glenzinski, D and Gold, M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Hardman, AD and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Hayashi, E and Heinrich, J and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway, L and Holscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes, R and Huston, J and Huth, J and Hylen, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and Jensen, H and Joshi, U and Kadel, RW and Kajfasz,
E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato,
Y and Keaffaber, TA and Keeble, L and Kelley, K and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian,
H and Keyvan, F and Kharadia, B and Kim, BJ and Kim, DH and Kim, HS and Kim,
SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Korytov, A and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuwabara, T and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca,
N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis,
JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lu, J and Lucchesi, D and Lukens, P and Lusin,
S and Lys, J and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin,
A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Mitsushio, H and Miyamoto, T and Miyashita, S and Moggi, N and Morita,
Y and Mueller, J and Mukherjee, A and Muller, T and Murat, P and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ninomiya, M and Nodulman, L and Oh, SH and Ohl, KE and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Oliveira, R and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Park, S and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips,
TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Romano, J and Rosenson, L and Roser, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scribano, A and Segler,
S and Seidel, S and Seiya, Y and Sganos, G and Shapiro, MD and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Snider,
FD and Song, T and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
A and Strahl, K and Strait, J and Strohmer, R and Stuart, D and Sullivan,
G and Soumarokov, A and Sumorok, K and Suzuki, J and Takada, T and Takahashi, T and Takano, T and Takikawa, K and Tamura, N and Tartarelli,
F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov, A and Tkaczyk,
S and Toback, D and Tollefson, K and Tollestrup, A and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Uemura, N and Ukegawa, F and Unal, G and Valls, J and Brink, SCVD and Vejcik, S and Velev, G and Vidal, R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, N and Wang, C and Wang, CH and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef, C and Yoshida, T and Yovanovitch, D and Yu, I and Yu, L and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, W and Zucchelli,
S},
Title = {Observation of Λ0b→J/ψ Λ at the
Fermilab proton-antiproton collider},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {55},
Number = {3},
Pages = {1142-1152},
Year = {1997},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.55.1142},
Abstract = {The decay Λ0b→J/ψ Λ is observed in 110 pb-1 of pp̄
collisions taken at √s=1.8 TeV. These data are used to
measure a Λ0b mass of 5621±4(stat)±3(syst) MeV/c2, and a
mass difference between the Λ0b and the B0 of
340±5(stat)±1(syst) MeV/c2. The production cross-section
times branching fraction for the decay Λ0b→J/ψ Λ
relative to that for the decay B0→J/ψ K0S has been
measured to be 0.27±0.12(stat)±0.05(syst).},
Doi = {10.1103/PhysRevD.55.1142},
Key = {fds308851}
}
@article{fds316862,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Operation and performance of the ATLAS semiconductor
tracker},
Journal = {Journal of Instrumentation},
Volume = {9},
Number = {8},
Pages = {P08009-P08009},
Publisher = {IOP Publishing},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1088/1748-0221/9/08/P08009},
Abstract = {The semiconductor tracker is a silicon microstrip detector
forming part of the inner tracking system of the ATLAS
experiment at the LHC. The operation and performance of the
semiconductor tracker during the first years of LHC running
are described. More than 99% of the detector modules were
operational during this period, with an average intrinsic
hit efficiency of (99.74±0.04)%. The evolution of the noise
occupancy is discussed, and measurements of the Lorentz
angle, d-ray production and energy loss presented. The
alignment of the detector is found to be stable at the
few-micron level over long periods of time. Radiation damage
measurements, which include the evolution of detector
leakage currents, are found to be consistent with
predictions and are used in the verification of radiation
background simulations.},
Doi = {10.1088/1748-0221/9/08/P08009},
Key = {fds316862}
}
@article{fds365364,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Verzini,
MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C},
Title = {Operation and performance of the ATLAS semiconductor tracker
in LHC Run 2},
Journal = {Journal of Instrumentation},
Volume = {17},
Number = {1},
Year = {2022},
Month = {January},
url = {http://dx.doi.org/10.1088/1748-0221/17/01/P01013},
Abstract = {The semiconductor tracker (SCT) is one of the tracking
systems for charged particles in the ATLAS detector. It
consists of 4088 silicon strip sensor modules. During Run 2
(2015-2018) the Large Hadron Collider delivered an
integrated luminosity of 156 fb−1 to the ATLAS experiment
at a centre-of-mass proton-proton collision energy of 13
TeV. The instantaneous luminosity and pile-up conditions
were far in excess of those assumed in the original design
of the SCT detector. Due to improvements to the data
acquisition system, the SCT operated stably throughout Run
2. It was available for 99.9% of the integrated luminosity
and achieved a data-quality efficiency of 99.85%. Detailed
studies have been made of the leakage current in SCT modules
and the evolution of the full depletion voltage, which are
used to study the impact of radiation damage to the
modules.},
Doi = {10.1088/1748-0221/17/01/P01013},
Key = {fds365364}
}
@article{fds365404,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Optimisation of large-radius jet reconstruction for the
ATLAS detector in 13 TeV proton–proton
collisions},
Journal = {European Physical Journal C},
Volume = {81},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09054-3},
Abstract = {Jet substructure has provided new opportunities for searches
and measurements at the LHC, and has seen continuous
development since the optimization of the large-radius jet
definition used by ATLAS was performed during Run 1. A range
of new inputs to jet reconstruction, pile-up mitigation
techniques and jet grooming algorithms motivate an
optimisation of large-radius jet reconstruction for ATLAS.
In this paper, this optimisation procedure is presented, and
the performance of a wide range of large-radius jet
definitions is compared. The relative performance of these
jet definitions is assessed using metrics such as their
pileup stability, ability to identify hadronically decaying
W bosons and top quarks with large transverse momenta. A new
type of jet input object, called a ‘unified flow object’
is introduced which combines calorimeter- and
inner-detector-based signals in order to achieve optimal
performance across a wide kinematic range. Large-radius jet
definitions are identified which significantly improve on
the current ATLAS baseline definition, and their modelling
is studied using pp collisions recorded by the ATLAS
detector at s=13TeV during 2017.},
Doi = {10.1140/epjc/s10052-021-09054-3},
Key = {fds365404}
}
@article{fds331628,
Author = {al, DAE},
Title = {Optimized search for single top quark production at the
Fermilab Tevatron},
Journal = {Phys. Rev.},
Volume = {D69},
Number = {5},
Pages = {052003},
Publisher = {American Physical Society (APS)},
Year = {2004},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.69.052003},
Abstract = {We use a neural-network technique to search for standard
model single-top-quark production in the 106Êpb-1 dataset
accumulated by the Collider Detector at Fermilab detector
during the 1992Ð1995 collider run (``run I''). Using a
sample of 64 W+1, 2, 3 jets events, we set a 95\% confidence
level upper limit of 24 pb on the W-gluon and W* combined
single-top cross section.},
Doi = {10.1103/PhysRevD.69.052003},
Key = {fds331628}
}
@article{fds366279,
Author = {Kruse, MC},
Title = {Past, present and future highlights in top and Higgs physics
from the CDF experiment},
Journal = {PARTICLES AND FIELDS},
Volume = {670},
Pages = {379-386},
Publisher = {AMER INST PHYSICS},
Editor = {Cotti, E and Mondragon, M and TavaresVelasco, G},
Year = {2003},
Month = {January},
ISBN = {0-7354-0135-7},
Key = {fds366279}
}
@article{fds17506,
Author = {M.C. Kruse},
Title = {Past, Present and Future Highlights in Top and Higgs Physics
from the CDF Experiment.},
Booktitle = {Particles and Fields, Tenth Mexican School on Particles and
Fields},
Publisher = {American Institute of Physics},
Editor = {U. Cotti and M. Mondragon and G. Tavares-Velasco},
Year = {2003},
Month = {Fall},
url = {http://library.fnal.gov/archive/test-preprint/fermilab-conf-03-050-e.shtml},
Abstract = {http://proceedings.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=APCPCS000670000001000379000001},
Key = {fds17506}
}
@article{fds315955,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Performance of b-jet identification in the ATLAS
experiment},
Journal = {Journal of Instrumentation},
Volume = {11},
Number = {4},
Pages = {P04008-P04008},
Publisher = {IOP Publishing},
Year = {2016},
Month = {April},
url = {http://dx.doi.org/10.1088/1748-0221/11/04/P04008},
Abstract = {The identification of jets containing b hadrons is important
for the physics programme of the ATLAS experiment at the
Large Hadron Collider. Several algorithms to identify jets
containing b hadrons are described, ranging from those based
on the reconstruction of an inclusive secondary vertex or
the presence of tracks with large impact parameters to
combined tagging algorithms making use of multi-variate
discriminants. An independent b-tagging algorithm based on
the reconstruction of muons inside jets as well as the
b-tagging algorithm used in the online trigger are also
presented. The b-jet tagging efficiency, the c-jet tagging
efficiency and the mistag rate for light flavour jets in
data have been measured with a number of complementary
methods. The calibration results are presented as scale
factors defined as the ratio of the efficiency (or mistag
rate) in data to that in simulation. In the case of b jets,
where more than one calibration method exists, the results
from the various analyses have been combined taking into
account the statistical correlation as well as the
correlation of the sources of systematic
uncertainty.},
Doi = {10.1088/1748-0221/11/04/P04008},
Key = {fds315955}
}
@article{fds308311,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Performance of jet substructure techniques for large-R jets
in proton-proton collisions at √s=7 TeV using the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {9},
Publisher = {Springer Nature},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2013)076},
Abstract = {This paper presents the application of a variety of
techniques to study jet substructure. The performance of
various modified jet algorithms, or jet grooming techniques,
for several jet types and event topologies is investigated
for jets with transverse momentum larger than 300 GeV.
Properties of jets subjected to the mass-drop filtering,
trimming, and pruning algorithms are found to have a reduced
sensitivity to multiple proton-proton interactions, are more
stable at high luminosity and improve the physics potential
of searches for heavy boosted objects. Studies of the
expected discrimination power of jet mass and jet
substructure observables in searches for new physics are
also presented. Event samples enriched in boosted W and Z
bosons and top-quark pairs are used to study both the
individual jet invariant mass scales and the efficacy of
algorithms to tag boosted hadronic objects. The analyses
presented use the full 2011 ATLAS dataset, corresponding to
an integrated luminosity of 4.7 ± 0.1 fb-1 from
proton-proton collisions produced by the Large Hadron
Collider at a centre-of-mass energy of √s=7 TeV. [Figure
not available: see fulltext.] © 2013 Cern for the benefit
of the ATLAS collaboration.},
Doi = {10.1007/JHEP09(2013)076},
Key = {fds308311}
}
@article{fds321148,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa,
M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton,
AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates,
RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer,
F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin,
PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker,
M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella,
G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford,
L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock,
I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Brown, J and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret,
MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini,
I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo,
F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G},
Title = {Performance of pile-up mitigation techniques for jets in
[Formula: see text] collisions at [Formula: see text] TeV
using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {11},
Pages = {581},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4395-z},
Abstract = {The large rate of multiple simultaneous proton-proton
interactions, or pile-up, generated by the Large Hadron
Collider in Run 1 required the development of many new
techniques to mitigate the adverse effects of these
conditions. This paper describes the methods employed in the
ATLAS experiment to correct for the impact of pile-up on jet
energy and jet shapes, and for the presence of spurious
additional jets, with a primary focus on the large
20.3 [Formula: see text] data sample collected at a
centre-of-mass energy of [Formula: see text]. The energy
correction techniques that incorporate sophisticated
estimates of the average pile-up energy density and tracking
information are presented. Jet-to-vertex association
techniques are discussed and projections of performance for
the future are considered. Lastly, the extension of these
techniques to mitigate the effect of pile-up on jet shapes
using subtraction and grooming procedures is
presented.},
Doi = {10.1140/epjc/s10052-016-4395-z},
Key = {fds321148}
}
@article{fds365362,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei,
D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
ATH and Arguin, JF and Argyropoulos, S},
Title = {Performance of the ATLAS Level-1 topological trigger in
Run 2},
Journal = {European Physical Journal C},
Volume = {82},
Number = {1},
Year = {2022},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09807-0},
Abstract = {During LHC Run 2 (2015–2018) the ATLAS Level-1
topological trigger allowed efficient data-taking by the
ATLAS experiment at luminosities up to 2.1× 1034 cm- 2s-
1, which exceeds the design value by a factor of two. The
system was installed in 2016 and operated in 2017 and 2018.
It uses Field Programmable Gate Array processors to select
interesting events by placing kinematic and angular
requirements on electromagnetic clusters, jets, τ-leptons,
muons and the missing transverse energy. It allowed to
significantly improve the background event rejection and
signal event acceptance, in particular for Higgs and
B-physics processes.},
Doi = {10.1140/epjc/s10052-021-09807-0},
Key = {fds365362}
}
@article{fds321284,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
M},
Title = {Performance of the ATLAS muon trigger in pp collisions at
[Formula: see text] TeV.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {3},
Pages = {120},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3325-9},
Abstract = {The performance of the ATLAS muon trigger system is
evaluated with proton-proton collision data collected in
2012 at the Large Hadron Collider at a centre-of-mass energy
of 8 TeV. It is primarily evaluated using events containing
a pair of muons from the decay of [Formula: see text]
bosons. The efficiency of the single-muon trigger is
measured for muons with transverse momentum [Formula: see
text] GeV, with a statistical uncertainty of less than
0.01 % and a systematic uncertainty of 0.6 %. The
[Formula: see text] range for efficiency determination is
extended by using muons from decays of [Formula: see text]
mesons, [Formula: see text] bosons, and top quarks. The muon
trigger shows highly uniform and stable performance. The
performance is compared to the prediction of a detailed
simulation.},
Doi = {10.1140/epjc/s10052-015-3325-9},
Key = {fds321284}
}
@article{fds365391,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA},
Title = {Performance of the ATLAS RPC detector and Level-1 muon
barrel trigger at √s = 13 TeV},
Journal = {Journal of Instrumentation},
Volume = {16},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1088/1748-0221/16/07/P07029},
Abstract = {The ATLAS experiment at the Large Hadron Collider (LHC)
employs a trigger system consisting of a first-level
hardware trigger (L1) and a software-based high-level
trigger. The L1 muon trigger system selects muon candidates,
assigns them to the correct LHC bunch crossing and
classifies them into one of six transverse-momentum
threshold classes. The L1 muon trigger system uses
resistive-plate chambers (RPCs) to generate the muon-induced
trigger signals in the central (barrel) region of the ATLAS
detector. The ATLAS RPCs are arranged in six concentric
layers and operate in a toroidal magnetic field with a
bending power of 1.5 to 5.5 Tm. The RPC detector consists of
about 3700 gas volumes with a total surface area of more
than 4000 m2. This paper reports on the performance of the
RPC detector and L1 muon barrel trigger using 60.8 fb-1 of
proton-proton collision data recorded by the ATLAS
experiment in 2018 at a centre-of-mass energy of 13 TeV.
Detector and trigger performance are studied using Z boson
decays into a muon pair. Measurements of the RPC detector
response, efficiency, and time resolution are reported.
Measurements of the L1 muon barrel trigger efficiencies and
rates are presented, along with measurements of the
properties of the selected sample of muon candidates.
Measurements of the RPC currents, counting rates and mean
avalanche charge are performed using zero-bias collisions.
Finally, RPC detector response and efficiency are studied at
different high voltage and front-end discriminator threshold
settings in order to extrapolate detector response to the
higher luminosity expected for the High Luminosity
LHC.},
Doi = {10.1088/1748-0221/16/07/P07029},
Key = {fds365391}
}
@article{fds375889,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Cardoso, MA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler,
A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Tame, ZPA and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Gupta, DB and Balasubramanian, R and Baldin,
EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas,
WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits,
M-S and Barklow, T and Baron, P and Moreno, DAB and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Navarro, LB and Barreiro, F and da
Costa, JBG and Barron, U and Teixeira, MGB and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Hurrell, LTB and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Kuutmann, EB and Berger, N and Bergmann, B and Beringer, J and Bernardi,
G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta,
P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Sola, JDB and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and de Renstrom, PAB and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Vazquez, CJB and Buzykaev, AR and Cabras, G and Urbán, SC and Cadamuro,
L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace,
N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Toro, RC and Camarda, S and Munoz, DC and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Bret, MC and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Argos, FC and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Garcia, LC and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini,
G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and El Moursli and RC and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A},
Title = {Performance of the reconstruction of large impact parameter
tracks in the inner detector of ATLAS},
Journal = {The European Physical Journal C},
Volume = {83},
Number = {11},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-12024-6},
Abstract = {<jats:title>Abstract</jats:title><jats:p>Searches for
long-lived particles (LLPs) are among the most promising
avenues for discovering physics beyond the Standard Model at
the Large Hadron Collider (LHC). However, displaced
signatures are notoriously difficult to identify due to
their ability to evade standard object reconstruction
strategies. In particular, the ATLAS track reconstruction
applies strict pointing requirements which limit sensitivity
to charged particles originating far from the primary
interaction point. To recover efficiency for LLPs decaying
within the tracking detector volume, the ATLAS Collaboration
employs a dedicated large-radius tracking (LRT) pass with
loosened pointing requirements. During Run 2 of the LHC, the
LRT implementation produced many incorrectly reconstructed
tracks and was therefore only deployed in small subsets of
events. In preparation for LHC Run 3, ATLAS has
significantly improved both standard and large-radius track
reconstruction performance, allowing for LRT to run in all
events. This development greatly expands the potential
phase-space of LLP searches and streamlines LLP analysis
workflows. This paper will highlight the above achievement
and report on the readiness of the ATLAS detector for
track-based LLP searches in Run 3.</jats:p>},
Doi = {10.1140/epjc/s10052-023-12024-6},
Key = {fds375889}
}
@article{fds308616,
Author = {Giromini, P and Happacher, F and Kim, MJ and Kruse, M and Pitts, K and Ptohos, F and Torre, S},
Title = {Phenomenological interpretation of the multi-muon events
reported by the CDF collaboration},
Journal = {Phys. Rev. D},
Year = {2008},
url = {http://arxiv.org/pdf/0810.5730},
Key = {fds308616}
}
@article{fds344673,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi,
A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Behari,
S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas,
J and Culbertson, R and Cully, JC and Daronco, S and Datta, M and D'Auria,
S and Davies, T and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher,
A and Lentdecker, GD and Lorenzo, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Dörr, C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg,
C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle,
T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy,
L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard,
PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
I and Sidoti, A},
Title = {Polarizations of J/ψ and ψ(2S) mesons produced in pp̄
collisions at s=1.96TeV},
Journal = {Physical Review Letters},
Volume = {99},
Number = {13},
Pages = {132001},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevLett.99.132001},
Abstract = {We have measured the polarizations of J/ψ and ψ(2S) mesons
as functions of their transverse momentum pT when they are
produced promptly in the rapidity range |y|<0.6 with pT
5GeV/c. The analysis is performed using a data sample with
an integrated luminosity of about 800pb-1 collected by the
CDF II detector. For both vector mesons, we find that the
polarizations become increasingly longitudinal as pT
increases from 5 to 30GeV/c. These results are compared to
the predictions of nonrelativistic quantum chromodynamics
and other contemporary models. The effective polarizations
of J/ψ and ψ(2S) mesons from B-hadron decays are also
reported. © 2007 The American Physical Society.},
Doi = {10.1103/PhysRevLett.99.132001},
Key = {fds344673}
}
@article{fds308620,
Author = {Abulencia, and A, and others},
Title = {Precise measurement of the top quark mass in the lepton+jets
topology at CDF II},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {18},
Pages = {182002},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.182002},
Abstract = {We present a measurement of the mass of the top quark from
proton-antiproton collisions recorded at the CDF experiment
in Run II of the Fermilab Tevatron. We analyze events from
the single lepton plus jets final state (t[overline
t]-->W+bW-[overline b]-->lnubq[overline q][prime][overline
b]). The top-quark mass is extracted using a direct
calculation of the probability density that each event
corresponds to the t[overline t] final state. The
probability is a function of both the mass of the top quark
and the energy scale of the calorimeter jets, which is
constrained in situ by the hadronic W boson mass. Using 167
events observed in 955 pb-1 of integrated luminosity, we
achieve the single most precise measurement of the top-quark
mass, 170.8$\pm$2.2(stat.)$\pm$1.4(syst.)
GeV/c2.},
Doi = {10.1103/physrevlett.99.182002},
Key = {fds308620}
}
@article{fds308276,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
M and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith,
D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A},
Title = {Precise measurement of the W -boson mass with the Collider
Detector at Fermilab},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.89.072003},
Abstract = {We present a measurement of the W-boson mass, MW, using data
corresponding to 2.2fb-1 of integrated luminosity collected
in pp̄ collisions at s=1.96TeV with the CDF II detector at
the Fermilab Tevatron. The selected sample of 470126 W→eν
candidates and 624708 W→μν candidates yields the
measurement MW=80387±12(stat)±15(syst)=80387±19MeV/c2.
This is the most precise single measurement of the W-boson
mass to date. © 2014 American Physical Society.},
Doi = {10.1103/PhysRevD.89.072003},
Key = {fds308276}
}
@article{fds308391,
Author = {Kotwal, AV and Collaboration, CDF},
Title = {Precise Measurement of the W-Boson Mass with the CDF II
Detector},
Journal = {Phys. Rev. Lett.},
Volume = {108},
Number = {15},
Pages = {151803},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.108.151803},
Abstract = {We have measured the W-boson mass M(W) using data
corresponding to 2.2 fb(-1) of integrated luminosity
collected in pp collisions at sqrt[s] = 1.96 TeV with
the CDF II detector at the Fermilab Tevatron collider.
Samples consisting of 470,126 W → eν candidates and
624,708 W → μν candidates yield the measurement M(W) =
80,387 ± 12(stat.) ± 15(syst.) = 80,387 ± 19 MeV/c2.
This is the most precise measurement of the W-boson mass to
date and significantly exceeds the precision of all previous
measurements combined.},
Doi = {10.1103/physrevlett.108.151803},
Key = {fds308391}
}
@article{fds308515,
Author = {Aaltonen, T and others},
Title = {Precision Measurement of the Ξ(3872) Mass in J/ψ π
+ π- Decays},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {15},
Pages = {152001},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.152001},
Abstract = {We present an analysis of the mass of the X(3872)
reconstructed via its decay to J/ψπ+π- using
2.4 fb-1 of integrated luminosity from pp̅ collisions
at sqrt[s]=1.96 TeV, collected with the CDF II detector
at the Fermilab Tevatron. The possible existence of two
nearby mass states is investigated. Within the limits of our
experimental resolution the data are consistent with a
single state, and having no evidence for two states we set
upper limits on the mass difference between two hypothetical
states for different assumed ratios of contributions to the
observed peak. For equal contributions, the 95% confidence
level upper limit on the mass difference is 3.6 MeV/c2.
Under the single-state model the X(3872) mass is measured to
be 3871.61 ± 0.16(stat) ± 0.19(syst) MeV/c2,
which is the most precise determination to
date.},
Doi = {10.1103/physrevlett.103.152001},
Key = {fds308515}
}
@article{fds308916,
Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman,
J},
Title = {Precision measurement of the prompt photon cross section in
pp-bar collisions at sqrt s =1.8 TeV.},
Journal = {Physical review letters},
Volume = {73},
Number = {20},
Pages = {2662-2666},
Publisher = {American Physical Society (APS)},
Year = {1994},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.73.2662},
Abstract = {A prompt photon cross section measurement from the Collider
Detector at Fermilab experiment is presented. Detector and
trigger upgrades, as well as 6 times the integrated
luminosity compared with our previous publication, have
contributed to a much more precise measurement and extended
PT range. As before, QCD calculations agree qualitatively
with the measured cross section, but the data has a steeper
slope than the calculations. © 1994 The American Physical
Society.},
Doi = {10.1103/physrevlett.73.2662},
Key = {fds308916}
}
@article{fds308643,
Author = {Abulencia, and A, and others},
Title = {Precision measurement of the top quark mass from dilepton
events at CDF II},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {3},
Pages = {031105},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.031105},
Abstract = {We report a measurement of the top-quark mass, Mt, in the
dilepton decay channel of t[overline t]-->b[script-l][prime]+nu[script-l][prime][overline
b][script-l]-[overline nu ][script-l] using an integrated
luminosity of 1.0 fb-1 of p[overline p] collisions collected
with the CDF II detector. We apply a method that convolutes
a leading-order matrix element with detector resolution
functions to form event-by-event likelihoods; we have
enhanced the leading-order description to describe the
effects of initial-state radiation. The joint likelihood is
the product of the likelihoods from 78 candidate events in
this sample, which yields a measurement of
Mt=164.5$\pm$3.9(stat.)$\pm$3.9(syst.) GeV/c2, the most
precise measurement of Mt in the dilepton
channel.},
Doi = {10.1103/PhysRevD.75.031105},
Key = {fds308643}
}
@article{fds308673,
Author = {Abulencia, and A, and others},
Title = {Precision top quark mass measurement in the lepton + jets
topology in p anti-p collisions at $\sqrt{s}=$
1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {2},
Pages = {022004},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.022004},
Abstract = {We report two measurements of the top quark mass M_top using
the CDF II detector at the Fermilab Tevatron in a 318 pb-1
data sample observed in the lepton + jets final state. One
method uses an event-based likelihood technique resulting in
M_top = 173.2+2.6_-2.4 (stat.) +/- 3.2 (syst.) GeV/c2 or
173.2+4.1_-40 GeV/c2. The second method reconstructs a top
quark mass in each event using the measured invariant mass
of the hadronically decaying W boson to constrain the jet
energy scale to obtain a value for M_top of 173.5+3.7_-3.6
(stat.) +/- 1.3 (syst.) GeV/c2 or 173.5+3.9_-3.8 GeV/c2. We
take the latter, which is more precise, as our
result.},
Doi = {10.1103/physrevlett.96.022004},
Key = {fds308673}
}
@article{fds308380,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Precision top-quark mass measurement at CDF.},
Journal = {Physical review letters},
Volume = {109},
Number = {15},
Pages = {152003},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.109.152003},
Abstract = {We present a precision measurement of the top-quark mass
using the full sample of Tevatron √s = 1.96 TeV
proton-antiproton collisions collected by the CDF II
detector, corresponding to an integrated luminosity of 8.7
fb(-1). Using a sample of tt¯ candidate events decaying
into the lepton+jets channel, we obtain distributions of the
top-quark masses and the invariant mass of two jets from the
W boson decays from data. We then compare these
distributions to templates derived from signal and
background samples to extract the top-quark mass and the
energy scale of the calorimeter jets with in situ
calibration. The likelihood fit of the templates from signal
and background events to the data yields the single
most-precise measurement of the top-quark mass,
M(top)=172.85±0.71(stat)±0.85(syst) GeV/c(2).},
Doi = {10.1103/physrevlett.109.152003},
Key = {fds308380}
}
@article{fds321201,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard,
CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman,
JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
Title = {Probing lepton flavour violation via neutrinoless [Formula:
see text] decays with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {232},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4041-9},
Abstract = {This article presents the sensitivity of the ATLAS
experiment to the lepton-flavour-violating decays of
[Formula: see text]. A method utilising the production of
[Formula: see text] leptons via [Formula: see text] decays
is used. This method is applied to the sample of
20.3 fb[Formula: see text] of <i>pp</i> collision data at a
centre-of-mass energy of 8 TeV collected by the ATLAS
experiment at the LHC in 2012. No event is observed passing
the selection criteria, and the observed (expected) upper
limit on the [Formula: see text] lepton branching fraction
into three muons, [Formula: see text], is [Formula: see
text] ([Formula: see text]) at 90 % confidence
level.},
Doi = {10.1140/epjc/s10052-016-4041-9},
Key = {fds321201}
}
@article{fds376064,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Probing the CP nature of the top–Higgs Yukawa coupling in
tt¯H and tH events with H→bb¯ decays using the ATLAS
detector at the LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {849},
Year = {2024},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2024.138469},
Abstract = {The CP properties of the coupling between the Higgs boson
and the top quark are investigated using 139 fb−1 of
proton–proton collision data recorded by the ATLAS
experiment at the LHC at a centre-of-mass energy of s=13
TeV. The CP structure of the top quark–Higgs boson Yukawa
coupling is probed in events with a Higgs boson decaying
into a pair of b-quarks and produced in association with
either a pair of top quarks, tt¯H, or a single top quark,
tH. Events containing one or two electrons or muons are used
for the measurement. Multivariate techniques are used to
select regions enriched in tt¯H and tH events, where
dedicated CP-sensitive observables are exploited. In an
extension of the Standard Model (SM) with a CP-odd admixture
in the top–Higgs Yukawa coupling, the mixing angle between
CP-even and CP-odd couplings is measured to be
α=11−73∘∘+52∘, compatible with the SM prediction
corresponding to α=0.},
Doi = {10.1016/j.physletb.2024.138469},
Key = {fds376064}
}
@article{fds308898,
Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and al, E},
Title = {Production in pp» collisions at s=1.8 TeV},
Journal = {Physical Review Letters},
Volume = {75},
Number = {24},
Pages = {4358-4363},
Year = {1995},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.75.4358},
Abstract = {We report on measurements of the (1S), (2S), and (3S)
differential, (d2 dPtdy)y=0, and integrated cross sections
in pp» collisions at s=1.8 TeV using a sample of 16.6 0.6
pb-1 collected by the Collider Detector at Fermilab. The
three resonances were reconstructed through the decay.
Comparison is made to a leading order QCD prediction. ©
1995 The American Physical Society.},
Doi = {10.1103/PhysRevLett.75.4358},
Key = {fds308898}
}
@article{fds308295,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Production of KS0, K*(892) and φ0(1020) in minimum bias
events and KS0 and Λ0 in jets in pp̄ collisions at
√s=1.96 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.88.092005},
Abstract = {We report measurements of the inclusive transverse momentum
(pT) distribution of centrally produced KS0, K±(892), and
φ0(1020) mesons up to pT=10 GeV/c in minimum bias events,
and KS0 and Λ0 particles up to pT=20 GeV/c in jets with
transverse energy between 25 and 160 GeV in pp̄ collisions.
The data were taken with the CDF II detector at the Fermilab
Tevatron at √s=1.96 TeV. We find that as pT increases, the
pT slopes of the three mesons (KS0, K±, and φ) are
similar. And using our previous Λ0 results from minimum
bias events, we show that the ratio of Λ0 to KS0 as a
function of pT in minimum bias events becomes similar to the
fairly constant ratio in jets at pT∼5 GeV/c. This suggests
that the particles with pTâ‰35 GeV/c in minimum bias
events are from "soft" jets, and that the pT slope of
particles in jets is insensitive to light quark flavor (u,
d, or s) and to the number of valence quarks. We also find
that for pT≠24 GeV relatively more Λ0 baryons are
produced in minimum bias events than in jets. © 2013
American Physical Society.},
Doi = {10.1103/PhysRevD.88.092005},
Key = {fds308295}
}
@article{fds341956,
Author = {Aaltonen, T and González, BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Cecco,
SD and Lorenzo, GD and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
ME and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa,
K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson,
GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel,
M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, C and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wen, A and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund,
AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka,
J},
Title = {Production of Λ0, Λ ̄0, Ξ ±, and
Ω± hyperons in pp̄ collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {1},
Year = {2012},
url = {http://dx.doi.org/10.1103/PhysRevD.86.012002},
Abstract = {We report a set of measurements of inclusive invariant p T
differential cross sections of Λ0, Λ ̄0, Ξ ±, and Ω ±
hyperons reconstructed in the central region with
pseudorapidity |η|<1 and p T up to 10GeV/c. Events are
collected with a minimum-bias trigger in pp̄ collisions at
a center-of-mass energy of 1.96 TeV using the CDF II
detector at the Tevatron Collider. As p T increases, the
slopes of the differential cross sections of the three
particles are similar, which could indicate a universality
of the particle production in p T. The invariant
differential cross sections are also presented for different
charged-particle multiplicity intervals. © 2012 American
Physical Society.},
Doi = {10.1103/PhysRevD.86.012002},
Key = {fds341956}
}
@article{fds308781,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman,
J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria,
S},
Title = {Production of χc1 and χc2 in pp̄
collisions at √s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {86},
Number = {18},
Pages = {3963-3968},
Year = {2001},
Month = {April},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.86.3963},
Abstract = {The charmonium system was studied by measuring the relative
cross sections of the Xc1 and Xc2 produced in pp collisions
at √ s = 1.8 TeV. As a result, the ratio of production
cross sections was established.},
Doi = {10.1103/PhysRevLett.86.3963},
Key = {fds308781}
}
@article{fds308562,
Author = {Aaltonen, T and others},
Title = {Production of ψ(2S) mesons in pp̅ collisions at 1.96
TeV},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {3},
Pages = {031103},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.031103},
Abstract = {We have measured the differential cross section for the
inclusive production of ψ(2S) mesons decaying to μ+μ-
that were produced in prompt or B-decay processes from pp̅
collisions at 1.96 TeV. These measurements have been made
using a data set from an integrated luminosity of
1.1 fb-1 collected by the CDF II detector at Fermilab.
For events with transverse momentum pT(ψ(2S))>2 GeV/c
and rapidity |y(ψ(2S))|<0.6 we measure the integrated
inclusive cross section σ(pp̅ →ψ(2S)X)·Br(ψ(2S)→μ+μ-)
to be 3.29 ± 0.04(stat) ± 0.32(syst) nb.},
Doi = {10.1103/PhysRevD.80.031103},
Key = {fds308562}
}
@article{fds375954,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF},
Title = {Production of ϒ(nS) mesons in Pb + Pb and pp collisions at
5.02 TeV},
Journal = {Physical Review C},
Volume = {107},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevC.107.054912},
Abstract = {A measurement of the production of vector bottomonium
states, ϒ(1S), ϒ(2S), and ϒ(3S), in Pb + Pb and pp
collisions at a center-of-mass energy per nucleon pair of
5.02 TeV is presented. The data correspond to integrated
luminosities of 1.38 nb-1 of Pb + Pb data collected in 2018,
0.44 nb-1 of Pb + Pb data collected in 2015, and 0.26 fb-1
of pp data collected in 2017 by the ATLAS detector at the
Large Hadron Collider. The measurements are performed in the
dimuon decay channel for transverse momentum pμμT < 30
GeV, absolute rapidity |yμμ| < 1.5, and Pb + Pb event
centrality 0-80%. The production rates of the three
bottomonium states in Pb + Pb collisions are compared with
those in pp collisions to extract the nuclear modification
factors as functions of event centrality, pμμT, and
|yμμ|. In addition, the suppression of the excited states
relative to the ground state is studied. The results are
compared with theoretical model calculations.},
Doi = {10.1103/PhysRevC.107.054912},
Key = {fds375954}
}
@article{fds308921,
Author = {Dracoulis, GD and Riess, F and Stuchbery, AE and Bark, RA and Gupta, SL and Baxter, AM and Kruse, M},
Title = {Properties of 15 2- states in 215Ra
and 217Th; evaluation of the 15 2- to
9 2+ E3 strength in N = 127 isotones},
Journal = {Nuclear Physics, Section A},
Volume = {493},
Number = {1},
Pages = {145-156},
Publisher = {Elsevier BV},
Year = {1989},
Month = {February},
url = {http://dx.doi.org/10.1016/0375-9474(89)90537-X},
Abstract = {The lifetime of the yrast 15 2- state in 215Ra was measured
using pulsed beams and γ-ray and electron techniques.
Transition multipolarities were established from measured
conversion coefficients. The B(E3) of the 15 2-→ 9 2+
transition is found to be considerably larger than
previously reported. A candidate for the corresponding
transition in 217Th was also observed. The E3 strength of
the 15 2-→ 9 2+ transition in the N = 127 isotones is
evaluated in the light of these and other recent results.
Interpretation in the framework of particle-octupole
vibration coupling requires a systematic lowering of the
core 3- vibration as proton pairs are added to 208Pb. ©
1989.},
Doi = {10.1016/0375-9474(89)90537-X},
Key = {fds308921}
}
@article{fds308896,
Author = {al, FAE},
Title = {Properties of high-mass multijet events at the fermilab
proton-antiproton collider},
Journal = {Phys. Rev. Lett.},
Volume = {75},
Number = {4},
Pages = {608-612},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.75.608},
Abstract = {The properties of two-, three-, four-, five-, and six-jet
events with multijet masses >600 GeV /c2 are compared with
QCD predictions. The shapes of the multijet-mass and
leading-jet-angular distributions are approximately
independent of jet multiplicity and are well described by
the NJETS matrix element calculation and the HERWIG parton
shower Monte Carlo predictions. The observed jet transverse
momentum distributions for three- and four-jet events
discriminate between the matrix element and parton shower
predictions, the data favoring the matrix element
calculation. © 1995 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.75.608},
Key = {fds308896}
}
@article{fds308854,
Author = {al, FAE},
Title = {Properties of jets in W boson events from 1.8 TeV
(p)over-bar-p collisions},
Journal = {Phys. Rev. Lett.},
Volume = {79},
Number = {24},
Pages = {4760-4765},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.79.4760},
Abstract = {We present a study of events with W bosons and hadronic jets
produced in p̄p collisions at a center of mass energy of
1.8 TeV. The data consist of 51 400 W± → e± decay
candidates from 108 pb-1 of integrated luminosity collected
using the CDF detector at the Fermilab Tevatron Collider.
Cross sections and jet production properties have been
measured for W + ≥1 to ≥4 jet events. The data are
compared to predictions of leading-order QCD matrix element
calculations with added gluon radiation and simulated parton
fragmentation.},
Doi = {10.1103/physrevlett.79.4760},
Key = {fds308854}
}
@article{fds308880,
Author = {al, FAE},
Title = {Properties of jets in Z boson events from 1.8 TeV
(p)over-bar-p collisions},
Journal = {Phys. Rev. Lett.},
Volume = {77},
Number = {3},
Pages = {448-453},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.77.448},
Abstract = {We present a study of events with Z bosons and hadronic jets
produced in ¯p p collisions at a center-of-mass energy of
1.8 TeV. The data consist of 6708 Z → e+e- decays from
106pb-1 of integrated luminosity collected using the CDF
detector at the Fermilab Tevatron Collider. The Z+ ≥ n jet
cross sections and jet production properties have been
measured for n = 1 to 4. The data are compared to
predictions of leading-order QCD matrix element calculations
with added gluon radiation and simulated parton
fragmentation. © 1996 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.77.448},
Key = {fds308880}
}
@article{fds308858,
Author = {al, FAE},
Title = {Properties of six-jet events with large six-jet mass at the
Fermilab proton-antiproton collider},
Journal = {Phys. Rev. D},
Volume = {56},
Number = {5},
Pages = {2532-2543},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.56.2532},
Abstract = {We describe the properties of six-jet events, with the
six-jet mass exceeding [Formula presented] produced at the
Fermilab proton-antiproton collider operating at a
center-of-mass energy of 1.8 TeV. Observed distributions for
a set of 20 multijet variables are compared with predictions
from the HERWIG QCD parton shower Monte Carlo program, the
NJETS leading order QCD matrix element Monte Carlo program,
and a phase-space model in which six-jet events are
distributed uniformly over the kinematically allowed region
of the six-body phase space. In general the QCD predictions
provide a good description of the observed six-jet
distributions. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevD.56.2532},
Key = {fds308858}
}
@article{fds308538,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
Title = {Publisher's Note: Search for hadronic decays of W and Z
bosons in photon events in pp̄ collisions at
s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {80},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.80.079901},
Doi = {10.1103/PhysRevD.80.079901},
Key = {fds308538}
}
@article{fds376830,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arbiol
Val, SJ and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Artoni,
G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal,
D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barel, MZ and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beaucamp, JY and Beauchemin, PH and Becherer, F and Bechtle, P and Beck,
HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry,
T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhalla, NK and Bhamjee, M and Bhatta, S and Bhattacharya,
DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco,
G and Biebel, O and Bielski, R and Biglietti, M and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borissov, G and Bortoletto,
D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans,
G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey,
PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev, AR and Cabrera Urbán and S and Cadamuro,
L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace,
N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty,
D and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili,
B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ},
Title = {Pursuit of paired dijet resonances in the Run 2 dataset with
ATLAS},
Journal = {Physical Review D},
Volume = {108},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevd.108.112005},
Doi = {10.1103/physrevd.108.112005},
Key = {fds376830}
}
@article{fds308874,
Author = {al, FAE},
Title = {Ratios of bottom meson branching fractions involving J/psi
mesons and determination of b quark fragmentation
fractions},
Journal = {Phys. Rev. D},
Volume = {54},
Number = {11},
Pages = {6596-6609},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevd.54.6596},
Abstract = {We report a measurement of the ratios of the decay rates of
the B+, B0, and B0s mesons into exclusive final states
containing a J/Ψ meson. The final states were selected from
19.6 pb-1 of pp collisions recorded by the Collider Detector
at Fermilab. These data are interpreted to determine the b
quark fragmentation fractions fu, fd, and fs. We also
determine the branching fractions for the decay modes
(formula presented). We discuss the implications of these
measurements to B meson decay models. © 1996 The American
Physical Society.},
Doi = {10.1103/physrevd.54.6596},
Key = {fds308874}
}
@article{fds365424,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Reconstruction and identification of boosted di-τ systems
in a search for Higgs boson pairs using 13 TeV proton-proton
collision data in ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {11},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2020)163},
Abstract = {In this paper, a new technique for reconstructing and
identifying hadronically decaying τ+τ− pairs with a
large Lorentz boost, referred to as the di-τ tagger, is
developed and used for the first time in the ATLAS
experiment at the Large Hadron Collider. A benchmark di-τ
tagging selection is employed in the search for resonant
Higgs boson pair production, where one Higgs boson decays
into a boosted bb¯ pair and the other into a boosted
τ+τ− pair, with two hadronically decaying τ-leptons in
the final state. Using 139 fb−1 of proton-proton collision
data recorded at a centre-of-mass energy of 13 TeV, the
efficiency of the di-τ tagger is determined and the
background with quark- or gluon-initiated jets misidentified
as di-τ objects is estimated. The search for a heavy,
narrow, scalar resonance produced via gluon-gluon fusion and
decaying into two Higgs bosons is carried out in the mass
range 1–3 TeV using the same dataset. No deviations from
the Standard Model predictions are observed, and 95%
confidence-level exclusion limits are set on this model.
[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP11(2020)163},
Key = {fds365424}
}
@article{fds308887,
Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cen, Y and Cervelli, F and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cunningham, JD and Daniels, T and DeJongh, F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dickson, M and Dittmann,
JR and Donati, S and Drucker, RB and Dunn, A and Einsweiler, K and Elias,
JE and Ely, R and Jr, EE and Eno, S and Errede, D and Errede, S and Fan, Q and Farhat, B and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman, J and Fry, A and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro,
M and Garfinkel, AF and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold,
M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Grewal, A and Groer, L and Grosso-Pilcher, C and Haber,
C and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Heinrich, J and Cronin-Hennessy, D and Hollebeek, R and Holloway, L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes,
R and Hurst, P and Huston, J and Huth, J and Hylen, J and Incagli, M and Incandela, J and Iso, H and Jensen, H and Jessop, CP and Joshi, U and Kadel, RW and Kajfasz, E and Kamon, T and Kaneko, T and Kardelis, DA and Kasha, H and Kato, Y and Keeble, L and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Loomis, C and Long, O and Loreti, M and Low, EH and Lu, J and Lucchesi, D and Luchini,
CB and Lukens, P and Lys, J and Maas, P and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Michail, G and Mikamo, S and Miller, M and Miller, R and Mimashi, T and Miscetti, S and Mishina, M and Mitsushio, H and Miyashita, S and Morita, Y and Moulding,
S and Mueller, J and Mukherjee, A and Muller, T and Musgrave, P and Nakae,
LF and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Nodulman, L and Ogawa, S and Oh, SH and Ohl, KE and Oishi, R and Okusawa,
T and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Park, S and Patrick, J and Pauletta, G and Paulini, M and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Plunkett, R and Pondrom, L and Produit, N and Proudfoot, J and Ptohos,
F and Punzi, G and Ragan, K and Rimondi, F and Ristori, L and Roach-Bellino, M and Robertson, WJ and Rodrigo, T and Romano, J and Rosenson, L and Sakumoto, WK and Saltzberg, D and Sansoni, A and Scarpine, V and Schindler, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schneider, O and Sciacca, GF and Scribano, A and Segler,
S and Seidel, S and Seiya, Y and Sganos, G and Sgolacchia, A and Shapiro,
M and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Smith, DA and Snider, FD and Song, L and Song, T and Spalding,
J and Spiegel, L and Sphicas, P and Stanco, L and Steele, J and Stefanini,
A and Strahl, K and Strait, J and Stuart, D and Sullivan, G and Sumorok, K and Swartz, RL and Takahashi, T and Takikawa, K and Tartarelli, F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, J and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov,
A and Tkaczyk, S and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Tseng, J and Turcotte, M and Turini, N and Uemura, N and Ukegawa, F and Unal, G and Brink, SCVD and III, SV and Vidal, R and Vondracek, M and Vucunic, D and Wagner, RG and Wagner, RL and Wainer, N and Walker, RC and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, G and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and III, WCW and Westhusing, T and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer,
BL and Wolinski, J and Wu, DY and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef,
C and Yoshida, T and Yovanovitch, D and Yu, I and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, S and Zhang, W and Zucchelli,
S},
Title = {Reconstruction of B0 → J/ψ
KS0 and measurement of ratios of
branching ratios involving B → J/ψK* and B+
→ J/ψK+},
Journal = {Physical Review Letters},
Volume = {76},
Number = {12},
Pages = {2015-2020},
Year = {1996},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.76.2015},
Abstract = {We report on the reconstruction of the decay mode B0 →
J/ψKS0 using 19.3 pb-1 of data collected by the Collider
Detector at Fermilab in p̄p collisions at s√ = 1.8 TeV. A
signal of 41.8 ± 6.9 events, with a signal-to-background
ratio of 9:1, is observed. Three additional decay modes B+
→ J/ψ K +, B0 → J/ψK* (892)0 and B+ → J/ψ K* (892)+
are reconstructed. We measure three ratios of branching
ratios, each one relative to the B+ → J/ψ K+ mode. We
also report the ratio of decay rates, Γ(B → J/ψ K*)/Γ(B
→ J/ψ K), for the vector-vector relative to the
vector-pseudoscalar modes, to be 1.32 ± 0.23(stat) ±
0.16(syst).},
Doi = {10.1103/PhysRevLett.76.2015},
Key = {fds308887}
}
@article{fds316858,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus,
M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
J},
Title = {Reconstruction of hadronic decay products of tau leptons
with the ATLAS experiment.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {295},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4110-0},
Abstract = {This paper presents a new method of reconstructing the
individual charged and neutral hadrons in tau decays with
the ATLAS detector. The reconstructed hadrons are used to
classify the decay mode and to calculate the visible
four-momentum of reconstructed tau candidates, significantly
improving the resolution with respect to the calibration in
the existing tau reconstruction. The performance of the
reconstruction algorithm is optimised and evaluated using
simulation and validated using samples of [Formula: see
text] and [Formula: see text]+jets events selected from
proton-proton collisions at a centre-of-mass energy
[Formula: see text], corresponding to an integrated
luminosity of 5 [Formula: see text].},
Doi = {10.1140/epjc/s10052-016-4110-0},
Key = {fds316858}
}
@article{fds308470,
Author = {Aaltonen, and T, and others},
Title = {Search for $R$-Parity Violating Decays of Sneutrinos to
$e\mu{}$, $\mu{}\tau{}$, and $e\tau{}$ Pairs in $pp[over
\ifmmode\bar\else\textasciimacron\fi{}]$ Collisions at
$\sqrt{s}=1.96\,\,TeV$},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {19},
Pages = {191801},
Publisher = {American Physical Society},
Year = {2010},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.191801},
Abstract = {We present a search for supersymmetric neutrino ν
production using the Tevatron pp collision data collected
with the CDF II detector and corresponding to an integrated
luminosity of 1 fb-1. We focus on the scenarios predicted by
the R-parity violating (RPV) supersymmetric models in which
sneutrinos decay to two charged leptons of different flavor.
With the data consistent with the standard model
expectations, we set upper limits on σ(pp→ν)×BR(ν→eμ,μτ,eτ)
and use these results to constrain the RPV couplings as a
function of the sneutrino mass.},
Doi = {10.1103/PhysRevLett.105.191801},
Key = {fds308470}
}
@article{fds308477,
Author = {Aaltonen, and T, and others},
Title = {Search for $WW$ and $WZ$ resonances decaying to electron,
missing $E_T$, and two jets in $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {24},
Pages = {241801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.241801},
Abstract = {http://arxiv.org/abs/1004.4946},
Doi = {10.1103/PhysRevLett.104.241801},
Key = {fds308477}
}
@article{fds308661,
Author = {Abulencia, and A, and others},
Title = {Search for $Z^\prime \to e^+ e^-$ using dielectron mass and
angular distribution},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {21},
Pages = {211801},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.211801},
Abstract = {We report results from a search for Z' bosons in high-mass
dielectron events produced in p anti-p collisions at
s**(1/2) = 1.96 TeV. The data were recorded with the CDF II
detector at the Fermilab Tevatron and correspond to an
integrated luminosity of 0.45 fb-1. To identify the Z' -->
e+ e- signal, both the dielectron invariant mass
distribution and the angular distribution of the electron
pair are used. No evidence for a signal is found, and 95\%
confidence level lower limits are set on the Z' mass for
several models.},
Doi = {10.1103/physrevlett.96.211801},
Key = {fds308661}
}
@article{fds308899,
Author = {al, FAE},
Title = {Search for 2nd-generation leptoquarks in p(p)over-bar
collisions at root-s=1.8 tev},
Journal = {Phys. Rev. Lett.},
Volume = {75},
Number = {6},
Pages = {1012-1016},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevLett.75.1012},
Abstract = {We present the results of a search for second generation
leptoquarks S2 using 19.3 pb-1 of data collected at the
Collider Detector at Fermilab (CDF) in pp» collisions at
s=1.8 TeV during the 1992 93 collider run. We have searched
for S2S2» pairs assuming that each leptoquark decays to a
muon + quark with a branching ratio. We find two candidate
events, consistent with an expected background of 1.11 0.48.
We obtain upper limits on (pp» S2S2») 2 as a function of
MS2. Using a Monte Carlo prediction for S2S2» pair
production, we exclude MS2<131GeV/c2 for =1 and MS2<96GeV/c2
for =0.5 at 95% C.L. © 1995 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.75.1012},
Key = {fds308899}
}
@article{fds321244,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
Title = {Search for a Charged Higgs Boson Produced in the
Vector-Boson Fusion Mode with Decay H(±)→W(±)Z using pp
Collisions at √s=8 TeV with the ATLAS
Experiment.},
Journal = {Physical review letters},
Volume = {114},
Number = {23},
Pages = {231801},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.114.231801},
Abstract = {A search for a charged Higgs boson, H(±), decaying to a
W(±) boson and a Z boson is presented. The search is based
on 20.3 fb(-1) of proton-proton collision data at a
center-of-mass energy of 8 TeV recorded with the ATLAS
detector at the LHC. The H(±) boson is assumed to be
produced via vector-boson fusion and the decays W(±)→qq'
and Z→e(+)e(-)/μ(+)μ(-) are considered. The search is
performed in a range of charged Higgs boson masses from 200
to 1000 GeV. No evidence for the production of an H(±)
boson is observed. Upper limits of 31-1020 fb at 95% C.L.
are placed on the cross section for vector-boson fusion
production of an H(±) boson times its branching fraction to
W(±)Z. The limits are compared with predictions from the
Georgi-Machacek Higgs triplet model.},
Doi = {10.1103/physrevlett.114.231801},
Key = {fds321244}
}
@article{fds321252,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for a CP-odd Higgs boson decaying to Zh in pp
collisions at √s=8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {744},
Pages = {163-183},
Publisher = {Elsevier BV},
Year = {2015},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2015.03.054},
Abstract = {A search for a heavy, CP-odd Higgs boson, A, decaying into a
Z boson and a 125 GeV Higgs boson, h, with the ATLAS
detector at the LHC is presented. The search uses
proton–proton collision data at a centre-of-mass energy of
8 TeV corresponding to an integrated luminosity of 20.3
fb−1. Decays of CP-even h bosons to ττ or bb pairs with
the Z boson decaying to electron or muon pairs are
considered, as well as h→bb decays with the Z boson
decaying to neutrinos. No evidence for the production of an
A boson in these channels is found and the 95% confidence
level upper limits derived for σ(gg→A)×BR(A→Zh)×BR(h→ff¯)
are 0.098–0.013 pb for f=τ and 0.57–0.014 pb for f=b in
a range of mA=220–1000 GeV. The results are combined and
interpreted in the context of two-Higgs-doublet
models.},
Doi = {10.1016/j.physletb.2015.03.054},
Key = {fds321252}
}
@article{fds308388,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Anzá, F and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Fuks, B and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Search for a dark matter candidate produced in association
with a single top quark in pp collisions at
√[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {20},
Pages = {201802},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.201802},
Abstract = {We report a new search for dark matter in a data sample of
an integrated luminosity of 7.7 fb-1 of Tevatron
pp[over ¯] collisions at √[s]=1.96 TeV, collected by
the CDF II detector. We search for production of a
dark-matter candidate, D, in association with a single top
quark. We consider the hadronic decay mode of the top quark
exclusively, yielding a final state of three jets with
missing transverse energy. The data are consistent with the
standard model; we thus set 95% confidence level upper
limits on the cross section of the process pp[over ¯]→t+D
as a function of the mass of the dark-matter candidate. The
limits are approximately 0.5 pb for a dark-matter particle
with mass in the range of 0-150 GeV/c2.},
Doi = {10.1103/physrevlett.108.201802},
Key = {fds308388}
}
@article{fds308296,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Search for a dijet resonance in events with jets and missing
transverse energy in pp̄ collisions at √s=1.96
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.88.092004},
Abstract = {We report on a search for a dijet resonance in events with
only two or three jets and a large imbalance in the total
event transverse momentum. This search is sensitive to the
possible production of a new particle in association with a
W or Z boson, where the boson decays leptonically with one
or more neutrinos in the final state. We use the full data
set collected by the CDF II detector at the Tevatron
collider at a proton-antiproton center-of-mass energy of
1.96 TeV. These data correspond to an integrated luminosity
of 9.1 fb -1. We study the invariant mass distribution of
the two jets with highest transverse energy. We find good
agreement between data and standard model background
expectations and measure the combined cross section for WW,
WZ, and ZZ production to be 13.8-2.7+3.0 pb. No significant
anomalies are observed in the mass spectrum, and 95%
credibility level upper limits are set on the production
rates of a potential new particle in association with a W or
Z boson. © 2013 American Physical Society.},
Doi = {10.1103/PhysRevD.88.092004},
Key = {fds308296}
}
@article{fds308520,
Author = {Aaltonen, T and others},
Title = {Search for a Fermiophobic Higgs Boson Decaying into
Diphotons in pp̅ Collisions at sqrt[s]=1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {6},
Pages = {061803},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.061803},
Abstract = {A search for a narrow diphoton mass resonance is presented
based on data from 3.0 fb-1 of integrated luminosity
from pp̅ collisions at sqrt[s]=1.96 TeV collected by
the CDF experiment. No evidence of a resonance in the
diphoton mass spectrum is observed, and upper limits are set
on the cross section times branching fraction of the
resonant state as a function of Higgs boson mass. The
resulting limits exclude Higgs bosons with masses below
106 GeV/c2 at a 95% Bayesian credibility level for one
fermiophobic benchmark model.},
Doi = {10.1103/physrevlett.103.061803},
Key = {fds308520}
}
@article{fds308802,
Author = {Collaboration, CDF},
Title = {Search for a Fourth-Generation Quark More Massive than the
Z0 Boson in pp Collisions at = 1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {84},
Number = {5},
Pages = {835},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevLett.84.835},
Abstract = {We present the results of a search for pair production of a
fourth-generation charge -1/3 quark (b′) in √s=1.8 TeV
pp¯ collisions using 88 pb−1 of data obtained with the
Collider Detector at Fermilab. We assume that both quarks
decay via the flavor-changing neutral current process
b′→bZ0 and that the b′ mass is greater than mZ+mb. We
studied the decay mode b′b′¯→Z0Z0bb¯ where one Z0
decays into e+e− or μ+μ− and the other decays
hadronically, giving a signature of two leptons plus jets.
An upper limit on the σpp¯→b′b′¯×[B(b′→bZ0)]2
is established as a function of the b′ mass. We exclude at
95% confidence level a b′ quark with mass between 100 and
199 GeV/c2 for B(b′→bZ0)=100%. © 2000 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.84.835},
Key = {fds308802}
}
@article{fds365399,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for a heavy Higgs boson decaying into a Z boson and
another heavy Higgs boson in the ℓℓbb and ℓℓWW final
states in pp collisions at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {5},
Year = {2021},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09117-5},
Abstract = {A search for a heavy neutral Higgs boson, A, decaying into a
Z boson and another heavy Higgs boson, H, is performed using
a data sample corresponding to an integrated luminosity of
139 fb- 1 from proton–proton collisions at s=13 TeV
recorded by the ATLAS detector at the LHC. The search
considers the Z boson decaying into electrons or muons and
the H boson into a pair of b-quarks or W bosons. The mass
range considered is 230–800 GeV for the A boson and
130–700 GeV for the H boson. The data are in good
agreement with the background predicted by the Standard
Model, and therefore 95% confidence-level upper limits for
σ×B(A→ZH)×B(H→bborH→WW) are set. The upper limits
are in the range 0.0062–0.380 pb for the H→ bb channel
and in the range 0.023–8.9 pb for the H→ WW channel. An
interpretation of the results in the context of
two-Higgs-doublet models is also given.},
Doi = {10.1140/epjc/s10052-021-09117-5},
Key = {fds365399}
}
@article{fds335594,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Search for a heavy Higgs boson decaying into a Z boson and
another heavy Higgs boson in the ℓℓbb final state in pp
collisions at √s= 13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {783},
Pages = {392-414},
Publisher = {Elsevier BV},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2018.07.006},
Abstract = {A search for a heavy neutral Higgs boson, A, decaying into a
Z boson and another heavy Higgs boson, H, is performed using
a data sample corresponding to an integrated luminosity of
36.1 fb−1 from proton–proton collisions at s=13 TeV
recorded in 2015 and 2016 by the ATLAS detector at the Large
Hadron Collider. The search considers the Z boson decaying
to electrons or muons and the H boson into a pair of
b-quarks. No evidence for the production of an A boson is
found. Considering each production process separately, the
95% confidence-level upper limits on the pp→A→ZH
production cross-section times the branching ratio H→bb
are in the range of 14–830 fb for the gluon–gluon fusion
process and 26–570 fb for the b-associated process for the
mass ranges 130–700 GeV of the H boson and 230–800 GeV
of the A boson. The results are interpreted in the context
of two-Higgs-doublet models.},
Doi = {10.1016/j.physletb.2018.07.006},
Key = {fds335594}
}
@article{fds321239,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G},
Title = {Search for a Heavy Neutral Particle Decaying to eμ, eτ, or
μτ in pp Collisions at sqrt[s]=8 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {115},
Number = {3},
Pages = {031801},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.115.031801},
Abstract = {This Letter presents a search for a heavy neutral particle
decaying into an opposite-sign different-flavor dilepton
pair, e^{±}μ^{∓}, e^{±}τ^{∓}, or μ^{±}τ^{∓}
using 20.3 fb^{-1} of pp collision data at
sqrt[s]=8 TeV collected by the ATLAS detector at the
LHC. The numbers of observed candidate events are compatible
with the standard model expectations. Limits are set on the
cross section of new phenomena in two scenarios: the
production of ν[over ˜]_{τ} in R-parity-violating
supersymmetric models and the production of a
lepton-flavor-violating Z^{'} vector boson.},
Doi = {10.1103/physrevlett.115.031801},
Key = {fds321239}
}
@article{fds308386,
Author = {Aaltonen, T and Adelman, J and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Rao, K and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Search for a heavy particle decaying to a top quark and a
light quark in pp ¯ collisions at √s=1.96
TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {21},
Pages = {211805},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.211805},
Abstract = {We present a search for a new heavy particle X produced in
association with a top quark, pp[over ¯]→t(X→t[over
¯]q) or pp[over ¯]→t[over ¯](X[over ¯]→tq[over ¯]),
where q stands for up quarks and down quarks. Such a
particle may explain the recent anomalous measurements of
top-quark forward-backward asymmetry. If the light-flavor
quark (q) is reconstructed as a jet (j), this gives a t[over
¯]+j or t+j resonance in tt[over ¯]+jet events, a
previously unexplored experimental signature. In a sample of
events with exactly one lepton, missing transverse momentum
and at least five jets, corresponding to an integrated
luminosity of 8.7 fb(-1) collected by the CDF II detector,
we find the data to be consistent with the standard model.
We set cross-section upper limits on the production (pp[over
¯]→Xt or X[over ¯]t[over ¯]) at 95% confidence level
from 0.61 pb to 0.02 pb for X masses ranging from 200
GeV/c(2) to 800 GeV/c(2), respectively.},
Doi = {10.1103/physrevlett.108.211805},
Key = {fds308386}
}
@article{fds308423,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De
Cecco, S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier,
L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez,
T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi,
L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt,
M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK},
Title = {Search for a heavy toplike quark in pp collisions at
√s=1.96 TeV.},
Journal = {Physical review letters},
Volume = {107},
Number = {26},
Pages = {261801},
Year = {2011},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.107.261801},
Abstract = {We present the results of a search for pair production of a
heavy toplike (t') quark decaying to Wq final states using
data corresponding to an integrated luminosity of 5.6 fb(-1)
collected by the CDF II detector in pp collisions at
√s=1.96 TeV. We perform parallel searches for t'→Wb and
t'→Wq (where q is a generic down-type quark) in events
containing a lepton and four or more jets. By performing a
fit to the two-dimensional distribution of total transverse
energy versus reconstructed t' quark mass, we set upper
limits on the t't' production cross section and exclude a
standard model fourth-generation t' quark decaying to Wb
(Wq) with mass below 358 (340) GeV/c(2) at 95%
C.L.},
Doi = {10.1103/physrevlett.107.261801},
Key = {fds308423}
}
@article{fds308367,
Author = {Aaltonen, T and Adelman, J and Lvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F},
Title = {Search for a heavy vector boson decaying to two gluons in
pp̄ collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.86.112002},
Abstract = {We present a search for a new heavy vector boson Z′ that
decays to gluons. Decays to on-shell gluons are suppressed,
leading to a dominant decay mode of Z′→g*g. We study the
case where the off-shell gluon g* converts to a pair of top
quarks, leading to a final state of tt̄g. In a sample of
events with exactly one charged lepton, large missing
transverse momentum and at least five jets, corresponding to
an integrated luminosity of 8.7fb-1 collected by the CDF II
detector, we find the data to be consistent with the
standard model. We set upper limits on the production cross
section times branching ratio of this chromophilic Z′ at
95% confidence level from 300 to 40 fb for Z′ masses
ranging from 400 to 1000GeV/c2, respectively. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.86.112002},
Key = {fds308367}
}
@article{fds308536,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey,
P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani,
M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo,
KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin,
PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen,
AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Movilla Fernandez and P and Mülmenstädt,
J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura,
K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman,
M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino,
G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Rekovic, V and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó,
O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker,
GL},
Title = {Search for a Higgs boson decaying to two W bosons at
CDF.},
Journal = {Physical review letters},
Volume = {102},
Number = {2},
Pages = {021802},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.102.021802},
Abstract = {We present a search for a Higgs boson decaying to two W
bosons in pp[over ] collisions at sqrt[s]=1.96 TeV
center-of-mass energy. The data sample corresponds to an
integrated luminosity of 3.0 fb;(-1) collected with the CDF
II detector. We find no evidence for production of a Higgs
boson with mass between 110 and 200 GeV/c;(2), and determine
upper limits on the production cross section. For the mass
of 160 GeV/c;(2), where the analysis is most sensitive, the
observed (expected) limit is 0.7 pb (0.9 pb) at 95% Bayesian
credibility level which is 1.7 (2.2) times the standard
model cross section.},
Doi = {10.1103/physrevlett.102.021802},
Key = {fds308536}
}
@article{fds308395,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Ray, J and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro,
A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri,
F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari,
M and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton,
O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov,
A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK},
Title = {Search for a Higgs boson in the diphoton final state in pp
collisions at sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {1},
Pages = {011801},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.108.011801},
Abstract = {A search for a narrow Higgs boson resonance in the diphoton
mass spectrum is presented based on data corresponding to
7.0 fb{-1} of integrated luminosity from pp collisions
at sqrt[s]=1.96 TeV collected by the CDF experiment. No
evidence of such a resonance is observed, and upper limits
are set on the cross section times branching ratio of the
resonant state as a function of Higgs boson mass. The limits
are interpreted in the context of the standard model and one
fermiophobic benchmark model where the data exclude
fermiophobic Higgs bosons with masses below
114 GeV/c{2} at a 95% Bayesian credibility
level.},
Doi = {10.1103/physrevlett.108.011801},
Key = {fds308395}
}
@article{fds308379,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M},
Title = {Search for a Higgs boson in the diphoton final state using
the full CDF data set from pp collisions at
s=1.96TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {717},
Number = {1-3},
Pages = {173-181},
Publisher = {Elsevier BV},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2012.08.051},
Abstract = {A search for a narrow Higgs boson resonance in the diphoton
mass spectrum is presented based on data corresponding to
10fb -1 of integrated luminosity collected by the CDF
experiment from proton-antiproton collisions at s=1.96TeV.
To increase the sensitivity of the search, we employ a
multivariate discriminant technique for the first time in
this channel at CDF. No evidence of signal is observed, and
upper limits are set on the cross section times branching
ratio of the resonant state as a function of the Higgs boson
mass. The limits are interpreted in the context of the
standard model with an expected (observed) limit on the
cross section times branching ratio of 9.9 (17.0) times the
standard model prediction at the 95% credibility level for a
Higgs boson mass of 125GeV/c 2. Moreover, a Higgs boson with
suppressed couplings to fermions is excluded for masses
below 114GeV/c 2 at the 95% credibility level. © 2012
Elsevier B.V.},
Doi = {10.1016/j.physletb.2012.08.051},
Key = {fds308379}
}
@article{fds308622,
Author = {Aaltonen, and T, and others},
Title = {Search for a high-mass diphoton state and limits on
Randall-Sundrum gravitons at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {17},
Pages = {171801},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.171801},
Abstract = {e have performed a search for new particles which decay to
two photons using 1.2 fb-1 of integrated luminosity from
p[overline p] collisions at sqrt(s)=1.96 TeV collected using
the CDF II detector at the Fermilab Tevatron. We find the
diphoton mass spectrum to be in agreement with the standard
model expectation, and set limits on the cross section times
branching ratio for the Randall-Sundrum graviton, as a
function of diphoton mass. We subsequently derive lower
limits for the graviton mass of 230 GeV/c2 and 850 GeV/c2,
at the 95\% confidence level, for coupling parameters
(k/[overline M]Pl) of 0.01 and 0.1, respectively.},
Doi = {10.1103/physrevlett.99.171801},
Key = {fds308622}
}
@article{fds308330,
Author = {The ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu,
E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y},
Title = {Search for a light charged Higgs boson in the decay channel
[Formula: see text] in [Formula: see text] events using
pp collisions at [Formula: see text] with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {6},
Pages = {2465},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2465-z},
Abstract = {A search for a charged Higgs boson (<i>H</i><sup>+</sup>) in
[Formula: see text] decays is presented, where one of the
top quarks decays via <i>t</i>→<i>H</i><sup>+</sup><i>b</i>,
followed by <i>H</i><sup>+</sup>→ two jets ([Formula: see
text]). The other top quark decays to <i>Wb</i>, where the
<i>W</i> boson then decays into a lepton
(<i>e</i>/<i>μ</i>) and a neutrino. The data were recorded
in <i>pp</i> collisions at [Formula: see text] by the ATLAS
detector at the LHC in 2011, and correspond to an integrated
luminosity of 4.7 fb<sup>-1</sup>. With no observation of a
signal, 95 % confidence level (CL) upper limits are set on
the decay branching ratio of top quarks to charged Higgs
bosons varying between 5 % and 1 % for
<i>H</i><sup>+</sup> masses between 90 GeV and 150 GeV,
assuming [Formula: see text].},
Doi = {10.1140/epjc/s10052-013-2465-z},
Key = {fds308330}
}
@article{fds321190,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Erbacher, R and Errede, S and Esham,
B},
Title = {Search for a low-mass neutral Higgs boson with suppressed
couplings to fermions using events with multiphoton final
states},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112010},
Abstract = {A search for a Higgs boson with suppressed couplings to
fermions, hf, assumed to be the neutral, lower-mass partner
of the Higgs boson discovered at the Large Hadron Collider,
is reported. Such a Higgs boson could exist in extensions of
the standard model with two Higgs doublets, and could be
produced via pp→H±hf→W∗hfhf→4γ+X, where H± is a
charged Higgs boson. This analysis uses all events with at
least three photons in the final state from
proton-antiproton collisions at a center-of-mass energy of
1.96 TeV collected by the Collider Detector at Fermilab,
corresponding to an integrated luminosity of 9.2 fb-1. No
evidence of a signal is observed in the data. Values of
Higgs-boson masses between 10 and 100 GeV/c2 are excluded at
95% Bayesian credibility.},
Doi = {10.1103/PhysRevD.93.112010},
Key = {fds321190}
}
@article{fds308390,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar,
C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann,
JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro,
P and Makhoul, K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín,
R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán,
J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang,
T},
Title = {Search for a low-mass standard model Higgs boson in the ττ
decay channel in pp collisions at sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {18},
Pages = {181804},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.181804},
Abstract = {We report on a search for the standard model Higgs boson
decaying into pairs of τ leptons in pp collisions produced
by the Tevatron at sqrt[s]=1.96 TeV. The analyzed data
sample was recorded by the CDFII detector and corresponds to
an integrated luminosity of 6.0 fb(-1). The search is
performed in the final state with one τ decaying
leptonically and the second one identified through its
semihadronic decay. Since no significant excess is observed,
a 95% credibility level upper limit on the production cross
section times branching ratio to the ττ final state is set
for hypothetical Higgs boson masses between 100 and
150 GeV/c2. For a Higgs boson of 120 GeV/c2 the
observed (expected) limit is 14.6 (15.3) the predicted
value.},
Doi = {10.1103/physrevlett.108.181804},
Key = {fds308390}
}
@article{fds308285,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
JF},
Title = {Search for a multi-Higgs-boson cascade in W+W
-bb̄ events with the ATLAS detector in pp
collisions at √s = 8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.89.032002},
Abstract = {A search is presented for new particles in an extension to
the Standard Model that includes a heavy Higgs boson (H0),
an intermediate charged Higgs-boson pair (H-), and a light
Higgs boson (h0). The analysis searches for events involving
the production of a single heavy neutral Higgs boson which
decays to the charged Higgs boson and a W boson, where the
charged Higgs boson subsequently decays into a W boson and
the lightest neutral Higgs boson decaying to a
bottom-antibottom-quark pair. Such a cascade results in a
W-boson pair and a bottom-antibottom-quark pair in the final
state. Events with exactly one lepton, missing transverse
momentum, and at least four jets are selected from a data
sample corresponding to an integrated luminosity of 20.3
fb-1, collected by the ATLAS detector in proton-proton
collisions at √s = 8 TeV at the LHC. The data are found to
be consistent with Standard Model predictions, and 95%
confidence-level upper limits are set on the product of
cross section and branching ratio. These limits range from
0.065 to 43 pb as a function of H0 and H- masses, with mh0
fixed at 125 GeV. © 2014 CERN, for the ATLAS
Collaboration.},
Doi = {10.1103/PhysRevD.89.032002},
Key = {fds308285}
}
@article{fds308658,
Author = {Abulencia, and A, and others},
Title = {Search for a neutral Higgs boson decaying to a W boson pair
in $p\bar{p}$ collisions at $\sqrt{s} =$
1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {97},
Number = {8},
Pages = {081802},
Year = {2006},
url = {http://arxiv.org/pdf/hep-ex/0605124},
Abstract = {We present the results of a search for standard model Higgs
boson production with decay to WW*, identified through the
leptonic final states e+e-nu-bar nu, e+/- mu-/+ nu-bar nu
and mu+ mu- nu-bar nu. This search uses 360 pb-1 of data
collected from p anti-p collisions at s**(1/2) = 1.96 TeV by
the upgraded Collider Detector at Fermilab (CDF II). We
observe no signal excess and set 95% confidence level upper
limits on the production cross section times branching ratio
for the Higgs boson to WW* or any new scalar particle with
similar decay products. These upper limits range from 5.5 to
3.2 pb for Higgs boson masses between 120 and 200
GeV/c2.},
Doi = {10.1103/physrevlett.97.081802},
Key = {fds308658}
}
@article{fds308458,
Author = {Aaltonen, and T, and al, E},
Title = {Search for a new heavy gauge boson ${W}^{$'${}}$ with event
signature $\mathrm{\text{electron}}+\mathrm{\text{missing}}$
transverse energy in $p\overline{p}$ collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {3},
Pages = {031102},
Publisher = {American Physical Society},
Year = {2011},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.83.031102},
Abstract = {We present a search for a new heavy charged vector boson
W′ decaying to an electron-neutrino pair in pp̄
collisions at a center-of-mass energy of 1.96 TeV. The data
were collected with the CDF II detector and correspond to an
integrated luminosity of 5.3fb-1. No significant excess
above the standard model expectation is observed and we set
upper limits on σ•B(W′→eν). Assuming standard model
couplings to fermions and the neutrino from the W′ boson
decay to be light, we exclude a W′ boson with mass less
than 1.12TeV/c2 at the 95% confidence level. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.83.031102},
Key = {fds308458}
}
@article{fds375895,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Pandya, HD and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Castillo, FL and Costanza, F and Delmastro, M and Di
Ciaccio, L and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo
Martinez, N and Poddar, G and Sanchez Pineda and A and Sauvan, E and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Li, T and Marchiori, G and Nakkalil, K and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
Gemmeren, P and Wamorkar, T and Wang, R and Zhang, J and Cheu, E and Cui,
Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost,
M},
Title = {Search for a new pseudoscalar decaying into a pair of muons
in events with a top-quark pair at Formula Presented with
the ATLAS detector},
Journal = {Physical Review D},
Volume = {108},
Number = {9},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.108.092007},
Abstract = {A search for a new pseudoscalar Formula Presented-boson
produced in events with a top-quark pair, where the Formula
Presented-boson decays into a pair of muons, is performed
using Formula Presented Formula Presented collision data
collected with the ATLAS detector at the LHC, corresponding
to an integrated luminosity of Formula Presented. The search
targets the final state where only one top quark decays to
an electron or muon, resulting in a signature with three
leptons Formula Presented and Formula Presented. No
significant excess of events above the Standard Model
expectation is observed and upper limits are set on two
signal models: Formula Presented and Formula Presented with
Formula Presented, Formula Presented, where Formula
Presented, in the mass ranges Formula Presented and Formula
Presented.},
Doi = {10.1103/PhysRevD.108.092007},
Key = {fds375895}
}
@article{fds321296,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
Title = {Search for a new resonance decaying to a W or
Z boson and a Higgs boson in the [Formula: see text]
final states with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {6},
Pages = {263},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3474-x},
Abstract = {A search for a new resonance decaying to a <i>W</i> or
<i>Z</i> boson and a Higgs boson in the [Formula: see text]
final states is performed using 20.3 fb[Formula: see text]
of <i>pp</i> collision data recorded at [Formula: see
text] 8 TeV with the ATLAS detector at the Large Hadron
Collider. The search is conducted by examining the
<i>WH</i> / <i>ZH</i> invariant mass distribution for a
localized excess. No significant deviation from the Standard
Model background prediction is observed. The results are
interpreted in terms of constraints on the Minimal Walking
Technicolor model and on a simplified approach based on a
phenomenological Lagrangian of Heavy Vector
Triplets.},
Doi = {10.1140/epjc/s10052-015-3474-x},
Key = {fds321296}
}
@article{fds365431,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
Title = {Search for a scalar partner of the top quark in the
all-hadronic tt¯ plus missing transverse momentum final
state at √s=13 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {8},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8102-8},
Abstract = {A search for direct pair production of scalar partners of
the top quark (top squarks or scalar third-generation
up-type leptoquarks) in the all-hadronic tt¯ plus missing
transverse momentum final state is presented. The analysis
of 139 fb - 1 of s=13 TeV proton–proton collision data
collected using the ATLAS detector at the LHC yields no
significant excess over the Standard Model background
expectation. To interpret the results, a supersymmetric
model is used where the top squark decays via
t~→t(∗)χ~10, with t(∗) denoting an on-shell
(off-shell) top quark and χ~10 the lightest neutralino.
Three specific event selections are optimised for the
following scenarios. In the scenario where mt~>mt+mχ~10,
top squark masses are excluded in the range 400–1250 GeV
for χ~10 masses below 200 GeV at 95% confidence level. In
the situation where mt~∼mt+mχ~10, top squark masses in
the range 300–630 GeV are excluded, while in the case
where mt~<mW+mb+mχ~10 (with mt~-mχ~10≥5 GeV),
considered for the first time in an ATLAS all-hadronic
search, top squark masses in the range 300–660 GeV are
excluded. Limits are also set for scalar third-generation
up-type leptoquarks, excluding leptoquarks with masses below
1240 GeV when considering only leptoquark decays into a top
quark and a neutrino.},
Doi = {10.1140/epjc/s10052-020-8102-8},
Key = {fds365431}
}
@article{fds308516,
Author = {Aaltonen, T and others},
Title = {Search for a Standard Model Higgs Boson in WH→ℓvbb̅ in
pp̅ Collisions at sqrt[s] =1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {10},
Pages = {101802},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.101802},
Abstract = {We present a search for a standard model Higgs boson
produced in association with a W boson using 2.7 fb-1
of integrated luminosity of pp̅ collision data taken at
sqrt[s]=1.96 TeV. Limits on the Higgs boson production
rate are obtained for masses between 100 and
150 GeV/c2. Through the use of multivariate techniques,
the analysis achieves an observed (expected) 95% confidence
level upper limit of 5.6 (4.8) times the theoretically
expected production cross section for a standard model Higgs
boson with a mass of 115 GeV/c2.},
Doi = {10.1103/physrevlett.103.101802},
Key = {fds308516}
}
@article{fds330940,
Author = {Collaboration, CDF},
Title = {Search for a Technicolor čT Particle in Events with a
Photon and a b-quark Jet at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {83},
Number = {16},
Pages = {3124},
Publisher = {American Physical Society (APS)},
Year = {1999},
url = {http://dx.doi.org/10.1103/PhysRevLett.83.3124},
Abstract = {If the technicolor ω particle exists, a likely decay mode
is ω →γπ , followed by π →bb¯, yielding the
signature γbb¯. We have searched 85pb of data collected by
the CDF experiment at the Fermilab Tevatron for events with
a photon and two jets, where one of the jets must contain a
secondary vertex implying the presence of a b quark. We find
no excess of events above standard model expectations. We
express the result as an exclusion region in the M −M mass
plane. © 1999 The American Physical Society. T T T T ωT
πT −1},
Doi = {10.1103/PhysRevLett.83.3124},
Key = {fds330940}
}
@article{fds308338,
Author = {Aaltonen, T and Adelman, J and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Johnstone, A and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Rao, K and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Truong, A and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund,
AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Search for a two-Higgs-boson doublet using a simplified
model in pp collisions at sqrt[s] = 1.96
TeV.},
Journal = {Physical review letters},
Volume = {110},
Number = {12},
Pages = {121801},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.110.121801},
Abstract = {We present a search for new particles in an extension to the
standard model that includes a heavy Higgs boson (H(0)), a
lighter charged Higgs boson (H(±)), and an even lighter
Higgs boson h(0), with decays leading to a W-boson pair and
a bottom-antibottom quark pair in the final state. We use
events with exactly one lepton, missing transverse momentum,
and at least four jets in data corresponding to an
integrated luminosity of 8.7 fb(-1) collected by the CDF II
detector in proton-antiproton collisions at sqrt[s]= 1.96
TeV. We find the data to be consistent with standard model
predictions and report the results in terms of a simplified
Higgs-cascade-decay model, setting 95% confidence level
upper limits on the product of cross section and branching
fraction from 1.3 pb to 15 fb as a function of H(0) and
H(±) masses for m(h)(0) = 126 GeV/c(2).},
Doi = {10.1103/physrevlett.110.121801},
Key = {fds308338}
}
@article{fds308435,
Author = {Aaltonen, and T, and al, E},
Title = {Search for a Very Light ${CP}$-Odd {H}iggs Boson in Top
Quark Decays from $p\overline{p}$ Collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {3},
Pages = {031801},
Publisher = {American Physical Society},
Year = {2011},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.031801},
Abstract = {We present the results of a search for a very light CP-odd
Higgs boson a(1)(0) originating from top quark decays t →
H(±)b → W(±(*)) a(1)(0)b, and subsequently decaying into
τ+ τ-. Using a data sample corresponding to an integrated
luminosity of 2.7 fb(-1) collected by the CDF II
detector in pp collisions at 1.96 TeV, we perform a search
for events containing a lepton, three or more jets, and an
additional isolated track with transverse momentum in the
range 3 to 20 GeV/c. Observed events are consistent
with background sources, and 95% C.L. limits are set on the
branching ratio of t → H(±)b for various masses of H(±)
and a(1)(0).},
Doi = {10.1103/PhysRevLett.107.031801},
Key = {fds308435}
}
@article{fds308750,
Author = {Collaboration, DAEACDF},
Title = {Search for a W' Boson Decaying to a Top and Bottom Quark
Pair in 1.8 TeV pp-bar Collisions},
Journal = {Physical Review Letters},
Volume = {90},
Number = {8},
Pages = {081802},
Year = {2003},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.90.081802},
Abstract = {We report the results of a search for a W' boson produced in
pp -bar collisions at a center-of-mass energy of 1.8 TeV
using a 106 pb-1 data sample recorded by the Collider
Detector at Fermilab. We observe no significant excess of
events above background for a W' boson decaying to a top and
bottom quark pair. In a model where this boson would mediate
interactions involving a massive right-handed neutrino ( nu
R) and have standard model strength couplings, we use these
data to exclude a W' boson with mass between 225 and 536
GeV/c2 at 95% confidence level for MW' >> M nu R and between
225 and 566 GeV/c2 at 95% confidence level for
MW'},
Doi = {10.1103/physrevlett.90.081802},
Key = {fds308750}
}
@article{fds330938,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Behrends, S and Belforte, S and Bellettini,
G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto,
G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng,
MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Dennino, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
R and Engels, E and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch, H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Guimaraes da Costa and J and Guo, RS and Haber, C and Hafen, E and Hahn,
SR and Hamilton, R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman,
KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman,
BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov,
A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino,
G and LeCompte, T and Lee, AM and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JA and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada,
H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CY and Niu, H and Nodulman, L and Nomerotski,
A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Partos,
D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara,
L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi,
F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
H and Trischuk, W and de Troconiz, JF and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and van Den Brink,
SC and Vejcik, S and Velev, G and Vidal, R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and Wester,
WC and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, S and Yao, W and Yasuoka, K and Yeh,
GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S and C D F Collaboration},
Title = {Search for a W' boson via the decay mode W'-->munumu in 1.8
TeV pp collisions.},
Journal = {Physical review letters},
Volume = {84},
Number = {25},
Pages = {5716-5721},
Year = {2000},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.84.5716},
Abstract = {We report the results of a search for a W' boson produced in
pp collisions at a center-of-mass energy of 1.8 TeV using a
107 pb-1 data sample recorded by the Collider Detector at
Fermilab. We consider the decay channel W'-->&munumu and
search for anomalous production of high transverse mass
munumu lepton pairs. We observe no excess of events above
background and set limits on the rate of W' boson production
and decay relative to standard model W boson production and
decay using a fit of the transverse mass distribution
observed. If we assume standard model strength couplings of
the W' boson to quark and lepton pairs, we exclude a W'
boson with invariant mass less than 660 GeV/c2 at 95%
confidence level.},
Doi = {10.1103/physrevlett.84.5716},
Key = {fds330938}
}
@article{fds321204,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
J},
Title = {Search for an additional, heavy Higgs boson in the [Formula:
see text] decay channel at [Formula: see text] in [Formula:
see text] collision data with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {45},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3820-z},
Abstract = {A search is presented for a high-mass Higgs boson in the
[Formula: see text], [Formula: see text], [Formula: see
text], and [Formula: see text] decay modes using the ATLAS
detector at the CERN Large Hadron Collider. The search uses
proton-proton collision data at a centre-of-mass energy of
8 TeV corresponding to an integrated luminosity of
20.3 fb[Formula: see text]. The results of the search are
interpreted in the scenario of a heavy Higgs boson with a
width that is small compared with the experimental mass
resolution. The Higgs boson mass range considered extends up
to [Formula: see text] for all four decay modes and down to
as low as 140 [Formula: see text], depending on the decay
mode. No significant excess of events over the Standard
Model prediction is found. A simultaneous fit to the four
decay modes yields upper limits on the production
cross-section of a heavy Higgs boson times the branching
ratio to [Formula: see text] boson pairs. 95 % confidence
level upper limits range from 0.53 pb at [Formula: see
text] GeV to 0.008 pb at [Formula: see text] GeV for the
gluon-fusion production mode and from 0.31 pb at [Formula:
see text] GeV to 0.009 pb at [Formula: see text] GeV for
the vector-boson-fusion production mode. The results are
also interpreted in the context of Type-I and Type-II
two-Higgs-doublet models.},
Doi = {10.1140/epjc/s10052-015-3820-z},
Key = {fds321204}
}
@article{fds314854,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Amako and K and Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for anomalous couplings in the W tb vertex from the
measurement of double differential angular decay rates of
single top quarks produced in the t-channel with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {4},
Pages = {1-46},
Publisher = {Springer Nature},
Year = {2016},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2016)023},
Abstract = {Abstract: The electroweak production and subsequent decay of
single top quarks is determined by the properties of the Wtb
vertex. This vertex can be described by the complex
parameters of an effective Lagrangian. An analysis of
angular distributions of the decay products of single top
quarks produced in the t -channel constrains these
parameters simultaneously. The analysis described in this
paper uses 4.6 fb−1 of proton-proton collision data at
(Formula presented.) TeV collected with the ATLAS detector
at the LHC. Two parameters are measured simultaneously in
this analysis. The fraction f1 of decays containing
transversely polarised W bosons is measured to be 0.37 ±
0.07 (stat.⊕syst.). The phase δ− between amplitudes for
transversely and longitudinally polarised W bosons recoiling
against left-handed b-quarks is measured to be −0.014π ±
0.036π (stat.⊕syst.). The correlation in the measurement
of these parameters is 0.15. These values result in
two-dimensional limits at the 95% confidence level on the
ratio of the complex coupling parameters gR and VL, yielding
Re[gR/VL] ∈ [−0.36, 0.10] and Im[gR/VL] ∈ [−0.17,
0.23] with a correlation of 0.11. The results are in good
agreement with the predictions of the Standard Model.[Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP04(2016)023},
Key = {fds314854}
}
@article{fds308715,
Author = {Acosta, and D, and others},
Title = {Search for anomalous production of diphoton events with
missing transverse energy at CDF and limits on gauge-
mediated supersymmetry-breaking models},
Journal = {Phys. Rev.},
Volume = {D71},
Number = {3},
Pages = {031104},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.031104},
Abstract = {http://arxiv.org/abs/hep-ex/0410053},
Doi = {10.1103/PhysRevD.71.031104},
Key = {fds308715}
}
@article{fds308550,
Author = {Aaltonen, T and others},
Title = {Search for anomalous production of events with a photon,
jet, b-quark jet, and missing transverse
energy},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {5},
Pages = {052003},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.052003},
Abstract = {We present a signature-based search for the anomalous
production of events containing a photon, two jets, of which
at least one is identified as originating from a b quark,
and missing transverse energy (E̸T). The search uses data
corresponding to 2.0 fb-1 of integrated luminosity from
pp̅ collisions at a center-of-mass energy of
sqrt[s]=1.96 TeV, collected with the CDF II detector at
the Fermilab Tevatron. From 6.697 47×106 events with a
photon candidate with transverse energy ET>25 GeV,
we find 617 events with E̸T>25 GeV and two or more
jets with ET>15 GeV, at least one identified as
originating from a b quark, versus an expectation of 607
± 113 events. Increasing the requirement on E̸T to
50 GeV, we find 28 events versus an expectation of 30
± 11 events. We find no indications of
non-standard-model phenomena.},
Doi = {10.1103/PhysRevD.80.052003},
Key = {fds308550}
}
@article{fds308501,
Author = {Aaltonen, and T, and others},
Title = {Search for anomalous production of events with two photons
and additional energetic objects at CDF},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {5},
Pages = {052005},
Publisher = {American Physical Society},
Year = {2010},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.82.052005},
Abstract = {We present results of a search for anomalous production of
two photons together with an electron, muon, τ lepton,
missing transverse energy, or jets using pp̄ collision data
from 1.1-2.0fb-1 of integrated luminosity collected by the
Collider Detector at Fermilab (CDF). The event yields and
kinematic distributions are examined for signs of new
physics without favoring a specific model of new physics.
The results are consistent with the standard model
expectations. The search employs several new analysis
techniques that significantly reduce instrumental
backgrounds in channels with an electron and missing
transverse energy. © 2010 The American Physical
Society.},
Doi = {10.1103/PhysRevD.82.052005},
Key = {fds308501}
}
@article{fds308630,
Author = {Abulencia, and A, and others},
Title = {Search for anomalous production of multi-lepton events in $p
\bar{p}$ collisions at $\sqrt{s}$ = 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {13},
Pages = {131804},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.131804},
Abstract = {We report a search for the anomalous production of events
with multiple charged leptons in p[overline p] collisions at
sqrt(s)=1.96 TeV using a data sample corresponding to an
integrated luminosity of 346 pb-1 collected by the CDF II
detector at the Fermilab Tevatron. The search is divided
into three-lepton and four-or-more-lepton data samples. We
observe six events in the three-lepton sample and zero
events in the >=4-lepton sample. Both numbers of events are
consistent with standard model background expectations.
Within the framework of an R-parity-violating supergravity
model, the results are interpreted as mass limits on the
lightest neutralino (chi-tilde10) and chargino
(chi-tilde1[plus-minus]) particles. For one particular
choice of model parameters, the limits are
M(chi-tilde10)>110 GeV/c2 and M(chi-tilde1[plus-minus])>203
GeV/c2 at 95\% confidence level; the variation of these mass
limits with model parameters is presented.},
Doi = {10.1103/physrevlett.98.131804},
Key = {fds308630}
}
@article{fds308415,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Search for anomalous production of multiple leptons in
association with W and Z bosons at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.85.092001},
Abstract = {This paper presents a search for anomalous production of
multiple low-energy leptons in association with a W or Z
boson using events collected at the CDF experiment
corresponding to 5.1fb -1 of integrated luminosity. This
search is sensitive to a wide range of topologies with
low-momentum leptons, including those with the leptons near
one another. The observed rates of production of additional
electrons and muons are compared with the standard model
predictions. No indications of phenomena beyond the standard
model are found. A 95% confidence level limit is presented
on the production cross section for a benchmark model of
supersymmetric hidden-valley Higgs production. Particle
identification efficiencies are also provided to enable the
calculation of limits on additional models. © 2012 American
Physical Society.},
Doi = {10.1103/PhysRevD.85.092001},
Key = {fds308415}
}
@article{fds321262,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for anomalous production of prompt same-sign lepton
pairs and pair-produced doubly charged Higgs bosons with s
=8 TeV pp collisions using the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {3},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP03(2015)041},
Abstract = {Abstract: A low-background inclusive search for new physics
in events with same-sign dileptons is presented. The search
uses proton-proton collisions corresponding to 20.3 fb−1
of integrated luminosity taken in 2012 at a centre-of-mass
energy of 8 TeV with the ATLAS detector at the LHC. Pairs of
isolated leptons with the same electric charge and large
transverse momenta of the type e±e±, e±μ±, and μ±μ±
are selected and their invariant mass distribution is
examined. No excess of events above the expected level of
Standard Model background is found. The results are used to
set upper limits on the cross-sections for processes beyond
the Standard Model. Limits are placed as a function of the
dilepton invariant mass within a fiducial region
corresponding to the signal event selection criteria.
Exclusion limits are also derived for a specific model of
doubly charged Higgs boson production.[Figure not available:
see fulltext.]},
Doi = {10.1007/JHEP03(2015)041},
Key = {fds321262}
}
@article{fds308682,
Author = {Abulencia, and A, and others},
Title = {Search for anomalous semileptonic decay of heavy flavor
hadrons produced in association with a W boson at CDF
II},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {5},
Pages = {051101},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.73.051101},
Abstract = {We present a search for anomalous semileptonic decays of
heavy flavor hadrons produced in association with a W boson,
in proton-antiproton collisions at s**(1/2) = 1.96 TeV. We
use 162 pb-1 of data collected with the CDF II detector at
the Fermilab Tevatron Collider. We select events with one W
boson and at least one jet with an identified secondary
vertex. In the jets with a secondary vertex we look for a
semileptonic decay to a muon. We compare the number of jets
with both a secondary vertex and a semileptonic decay, and
the kinematic properties of these jets, with the standard
model expectation, and we set limits on the production cross
section of a B-like hadron with an anomalously high
semileptonic branching ratio.},
Doi = {10.1103/PhysRevD.73.051101},
Key = {fds308682}
}
@article{fds308751,
Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Bensinger, J and Beretvas, A and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Bromberg, C and Brozovic, M and Brubaker,
E and Bruner, N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers,
W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Colijn, AP and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson,
R},
Title = {Search for associated production of Y and vector boson in
pp̄ Collisions at √s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {90},
Number = {22},
Pages = {2218031-2218037},
Year = {2003},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.90.221803},
Abstract = {Associated production of υ and vector boson in pp̄
collisions at √s = 1.8 TeV were investigated. The CDF
detector was used in the analysis. The analysis showed that
υ(1S) mesons in association with W± or Z0 bosons were not
observed by the CDF detector.},
Doi = {10.1103/physrevlett.90.221803},
Key = {fds308751}
}
@article{fds308741,
Author = {Acousta, D and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli, M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat,
C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de
Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Dininno, M and De Pedis,
D and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and Doksus,
P and Dominguez, A and Donati, S and Donega, M and D'Onnofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan,
G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester,
S and Foster, GW and Franklin, M and Frisch, H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Gondcharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra,
Y and Goulianos, K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Guimaraes da Costa and J and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans,
D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Karagoz Unel and M and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Kongisberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin,
CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martiínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Moulik, T and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, A-S and Nigmanov, T and Nodulman, L and Oesterberg, K and Ogawa, T and Oh, S and Oh, YD and Ohsugi, T and Okusawa,
T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pitts, KT and Plager, C and Pompos, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio,
S and Ratnikov, F and Ray, H and Reichold, A and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson,
WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Sfiligoi, I and Shears,
T and Scribano, A and Scuri, F and Sefov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Shapiro, MD and Shepard, PF and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Somalwar, SV and Spalding, J and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Squillacioti, P and Stadie,
H},
Title = {Search for B0s-->micro+micro- and B0d-->micro+micro- decays
in pp collisions at square root s = 1.96
TeV.},
Journal = {Physical review letters},
Volume = {93},
Number = {3},
Pages = {032001},
Year = {2004},
Month = {July},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.93.032001},
Abstract = {We report on a search for B(0)(s)-->micro(+)micro(-) and
B(0)(d)-->micro(+)micro(-) decays in pp collisions at square
root of s=1.96 TeV using 171 pb(-1) of data collected by the
CDF II experiment at the Fermilab Tevatron Collider. The
decay rates of these rare processes are sensitive to
contributions from physics beyond the standard model. One
event survives all our selection requirements, consistent
with the background expectation. We derive branching ratio
limits of B(B(0)(s)-->micro(+)micro(-))<5.8x10(-7) and
B(B(0)(d)-->micro(+)micro(-))<1.5x10(-7) at 90% confidence
level.},
Doi = {10.1103/physrevlett.93.032001},
Key = {fds308741}
}
@article{fds308720,
Author = {al, DAE},
Title = {Search for B0s-->µ+µ- and B0d-->µ+µ- Decays in pp-bar
Collisions at sqrt[s]=1.96 TeV},
Journal = {Physical Review Letters},
Volume = {93},
Number = {5},
Pages = {032001},
Publisher = {American Physical Society (APS)},
Year = {2004},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.72.051104},
Abstract = {We report on a search for B0s-->µ+µ- and B0d-->µ+µ-
decays in pp-bar collisions at sqrt[s]=1.96 TeV using 171
pb-1 of data collected by the CDF II experiment at the
Fermilab Tevatron Collider. The decay rates of these rare
processes are sensitive to contributions from physics beyond
the standard model. One event survives all our selection
requirements, consistent with the background expectation. We
derive branching ratio limits of B(B0s--
>µ+µ-)µ+µ-)},
Doi = {10.1103/PhysRevD.72.051104},
Key = {fds308720}
}
@article{fds321157,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel,
C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El
Moursli, RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M},
Title = {Search for bottom squark pair production in proton-proton
collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {10},
Pages = {547},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4382-4},
Abstract = {The result of a search for pair production of the
supersymmetric partner of the Standard Model bottom quark
([Formula: see text]) is reported. The search uses
3.2 fb[Formula: see text] of <i>pp</i> collisions at
[Formula: see text] TeV collected by the ATLAS experiment
at the Large Hadron Collider in 2015. Bottom squarks are
searched for in events containing large missing transverse
momentum and exactly two jets identified as originating from
<i>b</i>-quarks. No excess above the expected Standard Model
background yield is observed. Exclusion limits at 95 %
confidence level on the mass of the bottom squark are
derived in phenomenological supersymmetric
<i>R</i>-parity-conserving models in which the [Formula: see
text] is the lightest squark and is assumed to decay
exclusively via [Formula: see text], where [Formula: see
text] is the lightest neutralino. The limits significantly
extend previous results; bottom squark masses up to 800
(840) GeV are excluded for the [Formula: see text] mass
below 360 (100) GeV whilst differences in mass above
100 GeV between the [Formula: see text] and the [Formula:
see text] are excluded up to a [Formula: see text] mass of
500 GeV.},
Doi = {10.1140/epjc/s10052-016-4382-4},
Key = {fds321157}
}
@article{fds308605,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and De
Lorenzo, G and Dell'orso, M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di
Ruzza, B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt,
J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson,
W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Koay, SA and Kondo,
K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus,
J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marino, C and Marino, CP and Martin,
A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín,
R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello,
M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna,
G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria,
A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J},
Title = {Search for Bs0 --> micro+ micro- and B0 --> micro+ micro-
decays with 2 fb-1 of pp collisions.},
Journal = {Physical review letters},
Volume = {100},
Number = {10},
Pages = {101802},
Year = {2008},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.100.101802},
Abstract = {We have performed a search for B(s)(0) --> micro(+) micro(-)
and B(0) --> micro(+) micro(-) decays in pp collisions at
square root s = 1.96 TeV using 2 fb(-1) of integrated
luminosity collected by the CDF II detector at the Fermilab
Tevatron Collider. The observed number of B(s)(0) and B0
candidates is consistent with background expectations. The
resulting upper limits on the branching fractions are
B(B(s)0) --> micro(+) micro(-)) <5.8 x 10(-8) and B(B(0) -->
micro(+) micro(-))<1.8 x 10(-8) at 95% C.L.},
Doi = {10.1103/physrevlett.100.101802},
Key = {fds308605}
}
@article{fds314163,
Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'orso, M and Deluca,
C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'errico,
M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati,
S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Sperka, D and Squillacioti, P and Stancari, M and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang, YC},
Title = {Search for Bs0→μ+μ- and
B0→μ+μ- decays with CDF
II},
Journal = {Physical Review Letters},
Volume = {107},
Number = {19},
Pages = {191801},
Year = {2011},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.191801},
Abstract = {A search has been performed for Bs0→μ+μ- and B0→μ+μ-
decays using 7fb-1 of integrated luminosity collected by the
CDF II detector at the Fermilab Tevatron collider. The
observed number of B0 candidates is consistent with
background-only expectations and yields an upper limit on
the branching fraction of B(B0→μ+μ-)<6.0×10-9 at 95%
confidence level. We observe an excess of Bs0 candidates.
The probability that the background processes alone could
produce such an excess or larger is 0.27%. The probability
that the combination of background and the expected standard
model rate of Bs0→μ+μ- could produce such an excess or
larger is 1.9%. These data are used to determine
B(Bs0→μ+μ-)=(1.8-0.9+1.1)×10 -8 and provide an upper
limit of B(Bs0→μ+μ -)<4.0×10-8 at 95% confidence
level. © 2011 American Physical Society.},
Doi = {10.1103/PhysRevLett.107.191801},
Key = {fds314163}
}
@article{fds308336,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Search for Bs0→μ+μ- and
B0→μ+μ- decays with the full CDF
Run II data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.87.072003},
Abstract = {We report on a search for Bs0→μ+μ- and B0→μ+μ-
decays using proton-antiproton collision data at √s=1.96
TeV corresponding to 10 fb-1 of integrated luminosity
collected by the CDF II detector at the Fermilab Tevatron
collider. The observed number of B0 candidates is consistent
with background-only expectations and yields an upper limit
on the branching fraction of B(B0→μ+μ-)<4.6×10-9 at 95%
confidence level. We observe an excess of Bs0 candidates.
The probability that the background processes alone could
produce such an excess or larger is 0.94%. The probability
that the combination of background and the expected standard
model rate of Bs0→μ+μ- could produce such an excess or
larger is 6.8%. These data are used to determine a branching
fraction B(Bs0→μ+μ-)=(1.3-0.7+0.9) ×10-8 and provide an
upper limit of B(Bs0→μ +μ-)<3.1×10-8 at 95% confidence
level. © 2013 American Physical Society.},
Doi = {10.1103/PhysRevD.87.072003},
Key = {fds308336}
}
@article{fds308906,
Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman,
J},
Title = {Search for charged bosons heavier than the W boson in pp-bar
collisions at sqrt s=1800 GeV.},
Journal = {Physical review letters},
Volume = {74},
Number = {15},
Pages = {2900-2904},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.74.2900},
Abstract = {We have searched for new, heavy, charged bosons W′ through
the decay W′→eν in pp̄ collisions at s=1.8 TeV. The
data used in the search represent 19.7 pb-1 collected by the
Collider Detector at Fermilab. Limits are placed on
σB(pp̄→W′→eν) as a function of MW′. Assuming
standard couplings of the W′ to fermions, we establish the
limit MW′>652 GeV /c2 (95% C.L.). © 1995 The American
Physical Society.},
Doi = {10.1103/physrevlett.74.2900},
Key = {fds308906}
}
@article{fds308863,
Author = {al, FAE},
Title = {Search for charged Higgs boson decays of the top quark using
hadronic decays of the tau lepton},
Journal = {Phys. Rev. Lett.},
Volume = {79},
Number = {3},
Pages = {357-362},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.357},
Abstract = {This Letter describes a direct search for charged Higgs
boson production in proton-antiproton collisions at
sqrt(s)=1.8 TeV recorded by the Collider Detector at
Fermilab. Two-Higgs-doublet extensions to the standard model
predict the existence of charged Higgs bosons. In such
models, the branching fraction for top quarks B(t → H b
→ tau nu b) can be large. This search uses the hadronic
decays of the tau lepton in this channel to significantly
extend previous limits on charged Higgs production. © 1997
The American Physical Society.},
Doi = {10.1103/PhysRevLett.79.357},
Key = {fds308863}
}
@article{fds308870,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Auchincloss, P and Azfar,
F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov,
S and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas,
A and Berge, JP and Berryhill, J and Bertolucci, S and Bhatti, A and Biery,
K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner,
A},
Title = {Search for charged Higgs boson decays of the top quark using
hadronic tau decays.},
Journal = {Physical review. D, Particles and fields},
Volume = {54},
Number = {1},
Pages = {735-742},
Year = {1996},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevd.54.735},
Abstract = {We present the result of a search for charged Higgs boson
decays of the top quark, produced in p-p collisions at
√s=1.8 TeV. When the charged Higgs boson is heavy and
decays to a τ lepton, which subsequently decays
hadronically, the resulting events have a unique signature:
large missing transverse energy and the low-charged-multiplicity
τ. Data collected in 1992 and 1993 at the Collider Detector
at Fermilab, corresponding to 18.7±0.7 pb-1, exclude new
regions of combined top quark and charged Higgs boson mass,
in extensions to the standard model with two Higgs doublets.
© 1996 The American Physical Society.},
Doi = {10.1103/physrevd.54.735},
Key = {fds308870}
}
@article{fds365395,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for charged Higgs bosons decaying into a top quark
and a bottom quark at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {6},
Year = {2021},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2021)145},
Abstract = {A search for charged Higgs bosons decaying into a top quark
and a bottom quark is presented. The data analysed
correspond to 139 fb−1 of proton-proton collisions at s =
13 TeV, recorded with the ATLAS detector at the LHC. The
production of a heavy charged Higgs boson in association
with a top quark and a bottom quark, pp → tbH+ → tbtb,
is explored in the H+ mass range from 200 to 2000 GeV using
final states with jets and one electron or muon. Events are
categorised according to the multiplicity of jets and
b-tagged jets, and multivariate analysis techniques are used
to discriminate between signal and background events. No
significant excess above the background-only hypothesis is
observed and exclusion limits are derived for the production
cross-section times branching ratio of a charged Higgs boson
as a function of its mass; they range from 3.6 pb at 200 GeV
to 0.036 pb at 2000 GeV at 95% confidence level. The results
are interpreted in the hMSSM and Mh125 scenarios. [Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP06(2021)145},
Key = {fds365395}
}
@article{fds314179,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos,
S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold,
H},
Title = {Search for charged Higgs bosons decaying via H±
→ τ±ν in fully hadronic final states using
pp collision data at √s = 8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {3},
Publisher = {Springer Nature},
Year = {2015},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2015)088},
Abstract = {Abstract: The results of a search for charged Higgs bosons
decaying to a τ lepton and a neutrino, H± → τ±ν, are
presented. The analysis is based on 19.5 fb−1 of
proton-proton collision data at s$$ \sqrt{s} $$ = 8 TeV
collected by the ATLAS experiment at the Large Hadron
Collider. Charged Higgs bosons are searched for in events
consistent with top-quark pair production or in associated
production with a top quark, depending on the considered H±
mass. The final state is characterised by the presence of a
hadronic τ decay, missing transverse momentum, b-tagged
jets, a hadronically decaying W boson, and the absence of
any isolated electrons or muons with high transverse
momenta. The data are consistent with the expected
background from Standard Model processes. A statistical
analysis leads to 95% confidence-level upper limits on the
product of branching ratios ℬ(t → bH±) × ℬ(H± →
τ±ν), between 0.23% and 1.3% for charged Higgs boson
masses in the range 80-160GeV. It also leads to 95%
confidence-level upper limits on the production cross
section times branching ratio, σ(pp → tH± + X) ×
ℬ(H± → τ±ν), between 0.76 pb and 4.5 fb, for
charged Higgs boson masses ranging from 180 GeV to 1000 GeV.
In the context of different scenarios of the Minimal
Supersymmetric Standard Model, these results exclude nearly
all values of tan β above one for charged Higgs boson
masses between 80 GeV and 160 GeV, and exclude a region of
parameter space with high tan β for H± masses between 200
GeV and 250 GeV.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP03(2015)088},
Key = {fds314179}
}
@article{fds308672,
Author = {Abulencia, and A, and others},
Title = {Search for charged Higgs bosons from top quark decays in p
anti-p collisions at $\sqrt{s}$ = 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {4},
Pages = {042003},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.042003},
Abstract = {We report the results of a search for a charged Higgs boson
in the decays of top quarks produced in p anti-p collisions
at a center-of-mass energy of 1.96 GeV. We use a data sample
corresponding to an integrated luminosity of 193 pb-1
collected by the upgraded Collider Detector at Fermilab. No
evidence for charged Higgs production is found, allowing 95%
C.L. upper limits to be placed on BR(t --> H+b) for
different charged Higgs decay scenarios. In addition, we
present in the MSSM (m_H+/-, tan B) plane the first
exclusion regions with radiative and Yukawa coupling
corrections.},
Doi = {10.1103/physrevlett.96.042003},
Key = {fds308672}
}
@article{fds308517,
Author = {Aaltonen, T and others},
Title = {Search for Charged Higgs Bosons in Decays of Top Quarks in
pp̅ Collisions at sqrt[s] =1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {10},
Pages = {101803},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.101803},
Abstract = {We report on the first direct search for charged Higgs
bosons decaying into cs̅ in tt̅ events produced by pp̅
collisions at sqrt[s]=1.96 TeV. The search uses a data
sample corresponding to an integrated luminosity of
2.2 fb-1 collected by the CDF II detector at Fermilab
and looks for a resonance in the invariant mass distribution
of two jets in the lepton+jets sample of tt̅ candidates. We
observe no evidence of charged Higgs bosons in top quark
decays. Hence, 95% upper limits on the top quark decay
branching ratio are placed at B(t→H+b)< 0.1 to 0.3 for
charged Higgs boson masses of 60 to 150 GeV/c2 assuming
B(H+→cs̅ )=1.0. The upper limits on B(t→H+b) are also
used as model-independent limits on the decay branching
ratio of top quarks to generic scalar charged bosons beyond
the standard model.},
Doi = {10.1103/physrevlett.103.101803},
Key = {fds308517}
}
@article{fds321203,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Search for charged Higgs bosons in the H± → tb
decay channel in pp collisions at √s = 8 TeV using the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {3},
Publisher = {Springer Nature},
Year = {2016},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2016)127},
Abstract = {Charged Higgs bosons heavier than the top quark and decaying
via H± → tb are searched for in proton-proton collisions
measured with the ATLAS experiment at (Formula presented.)
TeV corresponding to an integrated luminosity of 20.3fb−1.
The production of a charged Higgs boson in association with
a top quark, gb → tH±, is explored in the mass range 200
to 600 GeV using multi-jet final states with one electron or
muon. In order to separate the signal from the Standard
Model background, analysis techniques combining several
kinematic variables are employed. An excess of events above
the background-only hypothesis is observed across a wide
mass range, amounting to up to 2.4 standard deviations.
Upper limits are set on the gb → tH± production cross
section times the branching fraction BR(H± → tb).
Additionally, the complementary s-channel production, qq′
→ H±, is investigated through a reinterpretation of W′
→ tb searches in ATLAS. Final states with one electron or
muon are relevant for H± masses from 0.4 to 2.0 TeV,
whereas the all-hadronic final state covers the range 1.5 to
3.0 TeV. In these search channels, no significant excesses
from the predictions of the Standard Model are observed, and
upper limits are placed on the qq′ → H± production
cross section times the branching fraction BR(H± →
tb).},
Doi = {10.1007/JHEP03(2016)127},
Key = {fds321203}
}
@article{fds321611,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for charged Higgs bosons produced in association with
a top quark and decaying via H± → τν using
pp collision data recorded at √s=13 TeV by the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {759},
Pages = {555-574},
Publisher = {Elsevier BV},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2016.06.017},
Abstract = {Charged Higgs bosons produced in association with a single
top quark and decaying via H±→τν are searched for with
the ATLAS experiment at the LHC, using proton–proton
collision data at s=13 TeV corresponding to an integrated
luminosity of 3.2 fb−1. The final state is characterised
by the presence of a hadronic τ decay and missing
transverse momentum, as well as a hadronically decaying top
quark, resulting in the absence of high-transverse-momentum
electrons and muons. The data are found to be consistent
with the expected background from Standard Model processes.
A statistical analysis leads to 95% confidence-level upper
limits on the production cross section times branching
fraction, σ(pp→[b]tH±)×BR(H±→τν), between 1.9 pb
and 15 fb, for charged Higgs boson masses ranging from 200
to 2000 GeV. The exclusion limits for this search surpass
those obtained with the proton–proton collision data
recorded at s=8 TeV.},
Doi = {10.1016/j.physletb.2016.06.017},
Key = {fds321611}
}
@article{fds308343,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Joffe, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
S and Arik, E and Arik, M},
Title = {Search for charged Higgs bosons through the violation of
lepton universality in tt events using pp collision data at
√S=7 TeV with the ATLAS experiment},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {3},
Publisher = {Springer Nature},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP03(2013)076},
Abstract = {In several extensions of the Standard Model, the top quark
can decay into a bottom quark and a light charged Higgs
boson H +, t → bH +, in addition to the Standard Model
decay t → bW. Since W bosons decay to the three lepton
generations equally, while H + maypredominantlydecayinto
τν, charged Higgs bosons can be searched for using the
violation of lepton universality in top quark decays. The
analysis in this paper is based on 4.6 fb-1 of proton-proton
collision data at √s=7 TeV collected by the ATLAS
experiment at the Large Hadron Collider. Signatures
containing leptons (e or μ) and/or a hadronically decaying
τ (τ had) are used. Event yield ratios between e + τ had
and e + μ, as well as between μ + τ had andμ + e, final
states are measured in the data and compared to predictions
from simulations. This ratio-based method reduces the impact
of systematic uncertainties in the analysis. No significant
deviation from the Standard Model predictions is observed.
With the assumption that the branching fraction ℬ (H + →
τν) is 100%, upper limits in the range 3.2%-4.4% can be
placed on the branching fraction ℬ (t → bH +) for
charged Higgs boson masses m H+ in the range 90-140 GeV.
After combination with results from a search for charged
Higgs bosons in t\overline{t} decays using the τ had + jets
final state, upper limits on ℬ (t → bH +) can be set in
the range 0.8%-3.4%, for m H+ in the range 90-160
GeV.[Figure not available: see fulltext.] © 2013 Cern for
the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP03(2013)076},
Key = {fds308343}
}
@article{fds365383,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Zeid, OSA and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz,
VA and Pereira, RA and Arcangeletti, C},
Title = {Search for charged-lepton-flavour violation in Z-boson
decays with the ATLAS detector},
Journal = {Nature Physics},
Volume = {17},
Number = {7},
Pages = {819-825},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1038/s41567-021-01225-z},
Abstract = {Leptons with essentially the same properties apart from
their mass are grouped into three families (or flavours).
The number of leptons of each flavour is conserved in
interactions, but this is not imposed by fundamental
principles. Since the formulation of the standard model of
particle physics, the observation of flavour oscillations
among neutrinos has shown that lepton flavour is not
conserved in neutrino weak interactions. So far, there has
been no experimental evidence that this also occurs in
interactions between charged leptons. Such an observation
would be a sign of undiscovered particles or a yet unknown
type of interaction. Here the ATLAS experiment at the Large
Hadron Collider at CERN reports a constraint on
lepton-flavour-violating effects in weak interactions,
searching for Z-boson decays into a τ lepton and another
lepton of different flavour with opposite electric charge.
The branching fractions for these decays are measured to be
less than 8.1 × 10−6 (eτ) and 9.5 × 10−6 (μτ) at
the 95% confidence level using 139 fb−1 of proton–proton
collision data at a centre-of-mass energy of s=13TeV and
20.3 fb−1 at s=8TeV. These results supersede the limits
from the Large Electron–Positron Collider experiments
conducted more than two decades ago.},
Doi = {10.1038/s41567-021-01225-z},
Key = {fds365383}
}
@article{fds308836,
Author = {Collaboration, CDF},
Title = {Search for Chargino-Neutralino Associated Production at the
Fermilab Tevatron Collider},
Journal = {Phys. Rev. Lett.},
Volume = {80},
Number = {13},
Pages = {5275},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.5275},
Abstract = {We have searched in pp collisions at √s=1.8TeV for events
with three charged leptons and missing transverse energy. In
the minimal supersymmetric standard model, we expect
trilepton events from chargino-neutralino (√ √ ) pair
production, with subsequent decay into leptons. We observe
no candidate e e e , e e μ , e μ μ , or μ μ μ events
in 106pb integrated luminosity. We present limits on the sum
of the branching ratios times cross section for the four
channels: σ χ B(χ χ →3ℓ+X)<0.34pb, M χ81.5GeV/c ,
and M >82.2GeV/c for tan >=2, μ=-600GeV/c , and M =M . ©
1998 The American Physical Society. ± 0 + - ± + - ± ± +
- + - ± -1 ± 0 ± 0 ± 2 0 2 2 1 2 σ 1 2 1 2 χ 1 χ 2 q
g},
Doi = {10.1103/PhysRevLett.80.5275},
Key = {fds308836}
}
@article{fds308619,
Author = {Aaltonen, T and others},
Title = {Search for Chargino-Neutralino Production in $p\overline p$
Collisions at $\sqrt{s}$=1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {19},
Pages = {191806},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.191806},
Abstract = {We present a search for associated production of the
chargino and neutralino supersymmetric particles using up to
1.1 fb-1 of integrated luminosity collected by the CDF II
experiment at the Tevatron p[overline p] collider at
sqrt(s)=1.96 TeV. We analyze events with a large transverse
momentum imbalance and either three charged leptons or two
charged leptons of the same electric charge. The numbers of
observed events are consistent with standard model
expectations. Upper limits on the production cross section
are derived in different theoretical models.},
Doi = {10.1103/physrevlett.99.191806},
Key = {fds308619}
}
@article{fds308872,
Author = {al, FAE},
Title = {Search for chargino-neutralino production in p(p)over-bar
collisions at root s=1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {76},
Number = {23},
Pages = {4307-4311},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevLett.76.4307},
Abstract = {We have searched for chargino-neutralino production
(χ±1χ02) in 1.8 TeV pp collisions, followed by their
leptonic decays χ±1 → χ01ℓ±ν and
χ02→χ01ℓ+ℓ-. These trilepton events are expected
within a framework of the minimal supersymmetric standard
model (MSSM). In a 19.1pb-1 data sample collected with a
Collider Detector at Fermilab, no trilepton events were
observed. Upper limits on σ(pp → χ±1χ02)BR(χ±1→02→3ℓ
+ X) were obtained for various MSSM parameter space regions,
yielding new 95% confidence level lower limits for the
neutralino (χ02) mass which extend as high as 49GeV/c2. ©
1996 The American Physical Society.},
Doi = {10.1103/PhysRevLett.76.4307},
Key = {fds308872}
}
@article{fds308291,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Search for charginos nearly mass degenerate with the
lightest neutralino based on a disappearing-track signature
in pp collisions at √(s) = 8 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {11},
Pages = {112006-1-112006-23},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.88.112006},
Abstract = {A search is presented for direct chargino production based
on a disappearing-track signature using 20:3 fb-1 of
proton-proton collisions at √s = 8 TeV collected with the
ATLAS experiment at the LHC. In anomaly-mediated
supersymmetry breaking (AMSB) models, the lightest chargino
is nearly mass degenerate with the lightest neutralino and
its lifetime is long enough to be detected in the tracking
detectors by identifying decays that result in tracks with
no associated hits in the outer region of the tracking
system. Some models with supersymmetry also predict
charginos with a significant lifetime. This analysis attains
sensitivity for charginos with a lifetime between 0.1 and 10
ns, and significantly surpasses the reach of the LEP
experiments. No significant excess above the background
expectation is observed for candidate tracks with large
transverse momentum, and constraints on chargino properties
are obtained. In the AMSB scenarios, a chargino mass below
270 GeV is excluded at 95% confidence level.},
Doi = {10.1103/PhysRevD.88.112006},
Key = {fds308291}
}
@article{fds365368,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
Bella, L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos,
S},
Title = {Search for chargino–neutralino pair production in final
states with three leptons and missing transverse momentum in
√s=13 TeV pp collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {12},
Year = {2021},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09749-7},
Abstract = {A search for chargino–neutralino pair production in
three-lepton final states with missing transverse momentum
is presented. The study is based on a dataset of s=13 TeV
pp collisions recorded with the ATLAS detector at the LHC,
corresponding to an integrated luminosity of 139 fb - 1. No
significant excess relative to the Standard Model
predictions is found in data. The results are interpreted in
simplified models of supersymmetry, and statistically
combined with results from a previous ATLAS search for
compressed spectra in two-lepton final states. Various
scenarios for the production and decay of charginos (χ~1±)
and neutralinos (χ~20) are considered. For pure higgsino
χ~1±χ~20 pair-production scenarios, exclusion limits at
95% confidence level are set on χ~20 masses up to 210 GeV.
Limits are also set for pure wino χ~1±χ~20 pair
production, on χ~20 masses up to 640 GeV for decays via
on-shell W and Z bosons, up to 300 GeV for decays via
off-shell W and Z bosons, and up to 190 GeV for decays via
W and Standard Model Higgs bosons.},
Doi = {10.1140/epjc/s10052-021-09749-7},
Key = {fds365368}
}
@article{fds308355,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for contact interactions and large extra dimensions
in dilepton events from pp collisions at √s=7 TeV with the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.87.015010},
Abstract = {A search for nonresonant new phenomena, originating from
either contact interactions or large extra spatial
dimensions, has been carried out using events with two
isolated electrons or muons. These events, produced at the
LHC in proton-proton collisions at √s=7 TeV, were recorded
by the ATLAS detector. The data sample, collected throughout
2011, corresponds to an integrated luminosity of 4.9 and 5.0
fb-1 in the e+e - and μ+μ- channels, respectively. No
significant deviations from the Standard Model expectation
are observed. Using a Bayesian approach, 95% confidence
level lower limits ranging from 9.0 to 13.9 TeV are placed
on the energy scale of ℓℓqq contact interactions in the
left-left isoscalar model. Lower limits ranging from 2.4 to
3.9 TeV are also set on the string scale in large extra
dimension models. After combining these limits with results
from a similar search in the diphoton channel, slightly more
stringent limits are obtained.},
Doi = {10.1103/PhysRevD.87.015010},
Key = {fds308355}
}
@article{fds321366,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Search for contact interactions and large extra dimensions
in the dilepton channel using proton-proton collisions at
[Formula: see text] 8 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {12},
Pages = {3134},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3134-6},
Abstract = {A search is conducted for non-resonant new phenomena in
dielectron and dimuon final states, originating from either
contact interactions or large extra spatial dimensions. The
LHC 2012 proton-proton collision dataset recorded by the
ATLAS detector is used, corresponding to 20 fb[Formula: see
text] at [Formula: see text] = 8 TeV. The dilepton
invariant mass spectrum is a discriminating variable in both
searches, with the contact interaction search additionally
utilizing the dilepton forward-backward asymmetry. No
significant deviations from the Standard Model expectation
are observed. Lower limits are set on the [Formula: see
text] contact interaction scale [Formula: see text] between
15.4 TeV and 26.3 TeV, at the 95 % credibility level. For
large extra spatial dimensions, lower limits are set on the
string scale [Formula: see text] between 3.2 TeV to
5.0 TeV.},
Doi = {10.1140/epjc/s10052-014-3134-6},
Key = {fds321366}
}
@article{fds308365,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim,
A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for dark matter candidates and large extra dimensions
in events with a jet and missing transverse momentum with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {4},
Publisher = {Springer Nature},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2013)075},
Abstract = {A search for new phenomena in events with a high-energy jet
and large missing transverse momentum is performed using
data from proton-proton collisions at √s=7 TeV with the
ATLAS experiment at the Large Hadron Collider. Four
kinematic regions are explored using a dataset corresponding
to an integrated luminosity of 4.7 fb-1. No excess of events
beyond expectations from Standard Model processes is
observed, and limits are set on large extra dimensions and
the pair production of dark matter particles. © 2013 CERN,
for the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP04(2013)075},
Key = {fds308365}
}
@article{fds365415,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Search for dark matter in association with an energetic
photon in pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {2},
Year = {2021},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2021)226},
Abstract = {A search for dark matter is conducted in final states
containing a photon and missing transverse momentum in
proton-proton collisions at s = 13 TeV. The data, collected
during 2015–2018 by the ATLAS experiment at the CERN LHC,
correspond to an integrated luminosity of 139 fb−1. No
deviations from the predictions of the Standard Model are
observed and 95% confidence-level upper limits between 2.45
fb and 0.5 fb are set on the visible cross section for
contributions from physics beyond the Standard Model, in
different ranges of the missing transverse momentum. The
results are interpreted as 95% confidence-level limits in
models where weakly interacting dark-matter candidates are
pair-produced via an s-channel axial-vector or vector
mediator. Dark-matter candidates with masses up to 415 (580)
GeV are excluded for axial-vector (vector) mediators, while
the maximum excluded mass of the mediator is 1460 (1470)
GeV. In addition, the results are expressed in terms of 95%
confidence-level limits on the parameters of a model with an
axion-like particle produced in association with a photon,
and are used to constrain the coupling gaZγ of an
axion-like particle to the electroweak gauge bosons. [Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP02(2021)226},
Key = {fds365415}
}
@article{fds308287,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao
De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Buehrer, F and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
B and Chapman, JD and Chapman, JW and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov,
A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow,
BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba,
J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron,
ZH},
Title = {Search for dark matter in events with a hadronically
decaying W or Z boson and missing transverse momentum in pp
collisions at √s=8 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {112},
Number = {4},
Pages = {041802},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.112.041802},
Abstract = {A search is presented for dark matter pair production in
association with a W or Z boson in pp collisions
representing 20.3 fb(-1) of integrated luminosity at
√s=8 TeV using data recorded with the ATLAS detector
at the Large Hadron Collider. Events with a hadronic jet
with the jet mass consistent with a W or Z boson, and with
large missing transverse momentum are analyzed. The data are
consistent with the standard model expectations. Limits are
set on the mass scale in effective field theories that
describe the interaction of dark matter and standard model
particles, and on the cross section of Higgs production and
decay to invisible particles. In addition, cross section
limits on the anomalous production of W or Z bosons with
large missing transverse momentum are set in two fiducial
regions.},
Doi = {10.1103/physrevlett.112.041802},
Key = {fds308287}
}
@article{fds321345,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for dark matter in events with a Z boson and missing
transverse momentum in pp collisions at s =8TeV with the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.90.012004},
Abstract = {A search is presented for production of dark-matter
particles recoiling against a leptonically decaying Z boson
in 20.3fb-1 of pp collisions at s=8TeV with the ATLAS
detector at the Large Hadron Collider. Events with large
missing transverse momentum and two oppositely charged
electrons or muons consistent with the decay of a Z boson
are analyzed. No excess above the Standard Model prediction
is observed. Limits are set on the mass scale of the contact
interaction as a function of the dark-matter particle mass
using an effective field theory description of the
interaction of dark matter with quarks or with Z bosons.
Limits are also set on the coupling and mediator mass of a
model in which the interaction is mediated by a scalar
particle. © 2014 CERN, for the ATLAS Collaboration.},
Doi = {10.1103/PhysRevD.90.012004},
Key = {fds321345}
}
@article{fds321285,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, M and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas,
AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus,
M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov,
SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie,
MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck,
HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall,
AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci,
F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan,
JG},
Title = {Search for dark matter in events with heavy quarks and
missing transverse momentum in [Formula: see text]
collisions with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {2},
Pages = {92},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3306-z},
Abstract = {This article reports on a search for dark matter pair
production in association with bottom or top quarks in
[Formula: see text] of [Formula: see text] collisions
collected at [Formula: see text] TeV by the ATLAS detector
at the LHC. Events with large missing transverse momentum
are selected when produced in association with high-momentum
jets of which one or more are identified as jets containing
[Formula: see text]-quarks. Final states with top quarks are
selected by requiring a high jet multiplicity and in some
cases a single lepton. The data are found to be consistent
with the Standard Model expectations and limits are set on
the mass scale of effective field theories that describe
scalar and tensor interactions between dark matter and
Standard Model particles. Limits on the dark-matter-nucleon
cross-section for spin-independent and spin-dependent
interactions are also provided. These limits are
particularly strong for low-mass dark matter. Using a
simplified model, constraints are set on the mass of dark
matter and of a coloured mediator suitable to explain a
possible signal of annihilating dark matter.},
Doi = {10.1140/epjc/s10052-015-3306-z},
Key = {fds321285}
}
@article{fds365376,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin,
JF},
Title = {Search for dark matter in events with missing transverse
momentum and a Higgs boson decaying into two photons in pp
collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {10},
Year = {2021},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2021)013},
Abstract = {A search for dark-matter particles in events with large
missing transverse momentum and a Higgs boson candidate
decaying into two photons is reported. The search uses 139
fb−1 of proton-proton collision data collected at s = 13
TeV with the ATLAS detector at the CERN LHC between 2015 and
2018. No significant excess of events over the Standard
Model predictions is observed. The results are interpreted
by extracting limits on three simplified models that include
either vector or pseudoscalar mediators and predict a final
state with a pair of dark-matter candidates and a Higgs
boson decaying into two photons. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP10(2021)013},
Key = {fds365376}
}
@article{fds321222,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Search for Dark Matter in Events with Missing Transverse
Momentum and a Higgs Boson Decaying to Two Photons in pp
Collisions at sqrt[s]=8 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {115},
Number = {13},
Pages = {131801},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.115.131801},
Abstract = {Results of a search for new phenomena in events with large
missing transverse momentum and a Higgs boson decaying to
two photons are reported. Data from proton-proton collisions
at a center-of-mass energy of 8 TeV and corresponding to an
integrated luminosity of 20.3 fb^{-1} have been collected
with the ATLAS detector at the LHC. The observed data are
well described by the expected standard model backgrounds.
Upper limits on the cross section of events with large
missing transverse momentum and a Higgs boson candidate are
also placed. Exclusion limits are presented for models of
physics beyond the standard model featuring dark-matter
candidates.},
Doi = {10.1103/physrevlett.115.131801},
Key = {fds321222}
}
@article{fds308387,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Bai,
Y and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Fox, PJ and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harnik, R and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins,
W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon,
T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, C and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys,
J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paus, C and Pellett,
DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Search for dark matter in events with one jet and missing
transverse energy in pp¯ collisions at √s=1.96
TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {21},
Pages = {211804},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.211804},
Abstract = {We present the results of a search for dark matter
production in the monojet signature. We analyze a sample of
Tevatron pp[over ¯] collisions at √s=1.96 TeV
corresponding to an integrated luminosity of 6.7 fb(-1)
recorded by the CDF II detector. In events with large
missing transverse energy and one energetic jet, we find
good agreement between the standard model prediction and the
observed data. We set 90% confidence level upper limits on
the dark matter production rate. The limits are translated
into bounds on nucleon-dark matter scattering rates which
are competitive with current direct detection bounds on
spin-independent interaction below a dark matter candidate
mass of 5 GeV/c(2), and on spin-dependent interactions up to
masses of 200 GeV/c(2).},
Doi = {10.1103/physrevlett.108.211804},
Key = {fds308387}
}
@article{fds321143,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for dark matter produced in association with a
hadronically decaying vector boson in pp collisions at
√s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {763},
Pages = {251-268},
Publisher = {Elsevier BV},
Year = {2016},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2016.10.042},
Abstract = {A search is presented for dark matter produced in
association with a hadronically decaying W or Z boson using
3.2 fb−1 of pp collisions at s=13 TeV recorded by the
ATLAS detector at the Large Hadron Collider. Events with a
hadronic jet compatible with a W or Z boson and with large
missing transverse momentum are analysed. The data are
consistent with the Standard Model predictions and are
interpreted in terms of both an effective field theory and a
simplified model containing dark matter.},
Doi = {10.1016/j.physletb.2016.10.042},
Key = {fds321143}
}
@article{fds329808,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark,
MR},
Title = {Search for Dark Matter Produced in Association with a Higgs
Boson Decaying to bb[over ¯] Using 36 fb^{-1} of pp
Collisions at sqrt[s]=13 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {119},
Number = {18},
Pages = {181804},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.119.181804},
Abstract = {Several extensions of the standard model predict associated
production of dark-matter particles with a Higgs boson. Such
processes are searched for in final states with missing
transverse momentum and a Higgs boson decaying to a bb[over
¯] pair with the ATLAS detector using 36.1 fb^{-1} of
pp collisions at a center-of-mass energy of 13 TeV at the
LHC. The observed data are in agreement with the standard
model predictions and limits are placed on the associated
production of dark-matter particles and a Higgs
boson.},
Doi = {10.1103/physrevlett.119.181804},
Key = {fds329808}
}
@article{fds315437,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Search for dark matter produced in association with a Higgs
boson decaying to two bottom quarks in pp collisions at s =8
TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {93},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {April},
ISSN = {2470-0010},
url = {http://dx.doi.org/10.1103/PhysRevD.93.072007},
Abstract = {This article reports on a search for dark matter pair
production in association with a Higgs boson decaying to a
pair of bottom quarks, using data from 20.3 fb-1 of pp
collisions at a center-of-mass energy of 8 TeV collected by
the ATLAS detector at the LHC. The decay of the Higgs boson
is reconstructed as a high-momentum bb system with either a
pair of small-radius jets, or a single large-radius jet with
substructure. The observed data are found to be consistent
with the expected Standard Model backgrounds.
Model-independent upper limits are placed on the visible
cross sections for events with a Higgs boson decaying into
bb and large missing transverse momentum with thresholds
ranging from 150 to 400 GeV. Results are interpreted using a
simplified model with a Z′ gauge boson decaying into
different Higgs bosons predicted in a two-Higgs-doublet
model, of which the heavy pseudoscalar Higgs decays into a
pair of dark matter particles. Exclusion limits are also
presented for the mass scales of various effective field
theory operators that describe the interaction between dark
matter particles and the Higgs boson.},
Doi = {10.1103/PhysRevD.93.072007},
Key = {fds315437}
}
@article{fds375941,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Search for dark matter produced in association with a single
top quark and an energetic W boson in √s= 13 TeV pp
collisions with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11582-z},
Abstract = {This paper presents a search for dark matter, χ , using
events with a single top quark and an energetic W boson. The
analysis is based on proton–proton collision data
collected with the ATLAS experiment at s= 13 TeV during LHC
Run 2 (2015–2018), corresponding to an integrated
luminosity of 139 fb - 1 . The search considers final states
with zero or one charged lepton (electron or muon), at least
one b-jet and large missing transverse momentum. In
addition, a result from a previous search considering
two-charged-lepton final states is included in the
interpretation of the results. The data are found to be in
good agreement with the Standard Model predictions and the
results are interpreted in terms of 95% confidence-level
exclusion limits in the context of a class of dark matter
models involving an extended two-Higgs-doublet sector
together with a pseudoscalar mediator particle. The search
is particularly sensitive to on-shell production of the
charged Higgs boson state, H± , arising from the
two-Higgs-doublet mixing, and its semi-invisible decays via
the mediator particle, a: H±→ W±a(→ χχ) . Signal
models with H± masses up to 1.5 TeV and a masses up to 350
GeV are excluded assuming a tan β value of 1. For masses of
a of 150 (250) GeV, tan β values up to 2 are excluded for
H± masses between 200 (400) GeV and 1.5 TeV. Signals with
tan β values between 20 and 30 are excluded for H± masses
between 500 and 800 GeV.},
Doi = {10.1140/epjc/s10052-023-11582-z},
Key = {fds375941}
}
@article{fds365377,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Search for dark matter produced in association with a single
top quark in √s=13 TeV pp collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {10},
Year = {2021},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09566-y},
Abstract = {This paper presents a search for dark matter in the context
of a two-Higgs-doublet model together with an additional
pseudoscalar mediator, a, which decays into the dark-matter
particles. Processes where the pseudoscalar mediator is
produced in association with a single top quark in the
2HDM+a model are explored for the first time at the LHC.
Several final states which include either one or two charged
leptons (electrons or muons) and a significant amount of
missing transverse momentum are considered. The analysis is
based on proton–proton collision data collected with the
ATLAS experiment at s=13 TeV during LHC Run 2
(2015–2018), corresponding to an integrated luminosity of
139 fb - 1. No significant excess above the Standard Model
predictions is found. The results are expressed as 95%
confidence-level limits on the parameters of the signal
models considered.},
Doi = {10.1140/epjc/s10052-021-09566-y},
Key = {fds365377}
}
@article{fds365374,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S},
Title = {Search for dark matter produced in association with a
Standard Model Higgs boson decaying into b-quarks using the
full Run 2 dataset from the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2021)209},
Abstract = {The production of dark matter in association with Higgs
bosons is predicted in several extensions of the Standard
Model. An exploration of such scenarios is presented,
considering final states with missing transverse momentum
and b-tagged jets consistent with a Higgs boson. The
analysis uses proton-proton collision data at a
centre-of-mass energy of 13 TeV recorded by the ATLAS
experiment at the LHC during Run 2, amounting to an
integrated luminosity of 139 fb−1. The analysis, when
compared with previous searches, benefits from a larger
dataset, but also has further improvements providing
sensitivity to a wider spectrum of signal scenarios. These
improvements include both an optimised event selection and
advances in the object identification, such as the use of
the likelihood-based significance of the missing transverse
momentum and variable-radius track-jets. No significant
deviation from Standard Model expectations is observed.
Limits are set, at 95% confidence level, in two benchmark
models with two Higgs doublets extended by either a heavy
vector boson Z′ or a pseudoscalar singlet a and which both
provide a dark matter candidate χ. In the case of the
two-Higgs-doublet model with an additional vector boson
Z′, the observed limits extend up to a Z′ mass of 3 TeV
for a mass of 100 GeV for the dark matter candidate. The
two-Higgs-doublet model with a dark matter particle mass of
10 GeV and an additional pseudoscalar a is excluded for
masses of the a up to 520 GeV and 240 GeV for tan β = 1 and
tan β = 10 respectively. Limits on the visible
cross-sections are set and range from to 0.05 fb to 3.26 fb,
depending on the missing transverse momentum and b-quark jet
multiplicity requirements. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP11(2021)209},
Key = {fds365374}
}
@article{fds375887,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour,
G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr,
AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano
Hurrell, LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir,
M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir,
O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone,
A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin,
E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A},
Title = {Search for Dark Photons in Rare Z Boson Decays with the
ATLAS Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {25},
Pages = {251801},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.131.251801},
Abstract = {A search for events with a dark photon produced in
association with a dark Higgs boson via rare decays of the
standard model Z boson is presented, using 139 fb^{-1}
of sqrt[s]=13 TeV proton-proton collision data recorded
by the ATLAS detector at the Large Hadron Collider. The dark
boson decays into a pair of dark photons, and at least two
of the three dark photons must each decay into a pair of
electrons or muons, resulting in at least two same-flavor
opposite-charge lepton pairs in the final state. The data
are found to be consistent with the background prediction,
and upper limits are set on the dark photon's coupling to
the dark Higgs boson times the kinetic mixing between the
standard model photon and the dark photon, α_{D}ϵ^{2}, in
the dark photon mass range of [5, 40] GeV except for the ϒ
mass window [8.8, 11.1] GeV. This search explores new
parameter space not previously excluded by other
experiments.},
Doi = {10.1103/physrevlett.131.251801},
Key = {fds375887}
}
@article{fds308358,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
ATH and Arfaoui, S and Arguin, JF and Arik, E},
Title = {Search for direct chargino production in anomaly-mediated
supersymmetry breaking models based on a disappearing-track
signature in pp collisions at √s=7TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {1},
Publisher = {Springer Nature},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP01(2013)131},
Abstract = {A search for direct chargino production in anomaly-mediated
supersymmetry breaking scenarios is performed in pp
collisions at √s=7TeV using 4.7 fb-1 of data collected
with the ATLAS experiment at the LHC. In these models, the
lightest chargino is predicted to have a lifetime long
enough to be detected in the tracking detectors of collider
experiments. This analysis explores such models by searching
for chargino decays that result in tracks with few
associated hits in the outer region of the tracking system.
The transverse-momentum spectrum of candidate tracks is
found to be consistent with the expectation from the
Standard Model background processes and constraints on
chargino properties are obtained. © 2013 CERN for the
benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP01(2013)131},
Key = {fds308358}
}
@article{fds321290,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
Title = {Search for direct pair production of a chargino and a
neutralino decaying to the 125 GeV Higgs boson in [Formula:
see text] TeV [Formula: see text] collisions with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {5},
Pages = {208},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3408-7},
Abstract = {A search is presented for the direct pair production of a
chargino and a neutralino [Formula: see text], where the
chargino decays to the lightest neutralino and the [Formula:
see text] boson, [Formula: see text], while the neutralino
decays to the lightest neutralino and the 125 GeV Higgs
boson, [Formula: see text]. The final states considered for
the search have large missing transverse momentum, an
isolated electron or muon, and one of the following: either
two jets identified as originating from bottom quarks, or
two photons, or a second electron or muon with the same
electric charge. The analysis is based on 20.3 [Formula:
see text] of [Formula: see text] proton-proton collision
data delivered by the Large Hadron Collider and recorded
with the ATLAS detector. Observations are consistent with
the Standard Model expectations, and limits are set in the
context of a simplified supersymmetric model.},
Doi = {10.1140/epjc/s10052-015-3408-7},
Key = {fds321290}
}
@article{fds321331,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for direct pair production of the top squark in
all-hadronic final states in proton-proton collisions at
√s = 8TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {9},
Pages = {1-51},
Publisher = {Springer Nature},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2014)015},
Abstract = {The results of a search for direct pair production of the
scalar partner to the top quark using an integrated
luminosity of 20.1 fb-1 of proton-proton collision data at
yfs = 8 TeV recorded with the ATLAS detector at the LHC are
reported. The top squark is assumed to decay via t → t
χ¯01 or t → b χ1 → bW(*)χ-01, where χ-01 (x1)
denotes the lightest neutralino (chargino) in supersymmetric
models. The search targets a fully-hadronic final state in
events with four or more jets and large missing transverse
momentum. No significant excess over the Standard Model
background prediction is observed, and exclusion limits are
reported in terms of the top squark and neutralino masses
and as a function of the branching fraction of t → t
χ-01. For a branching fraction of 100%, top squark masses
in the range 270-645 GeV are excluded for χ-01 masses below
30GeV. For a branching fraction of 50% to either t → t
χ-01 or t → b χ-01, and assuming the χ¯1 mass to be
twice the χ-01 mass, top squark masses in the range 250-550
GeV are excluded for χ-01 masses below 60
GeV.},
Doi = {10.1007/JHEP09(2014)015},
Key = {fds321331}
}
@article{fds308281,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Search for direct production of charginos and neutralinos in
events with three leptons and missing transverse momentum in
pv s = 8 TeV pp collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {4},
Pages = {1-52},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP04(2014)169},
Abstract = {A search for the direct production of charginos and
neutralinos in final states with three leptons and missing
transverse momentum is presented. The analysis is based on
20.3 fb-1 of vs = 8TeV proton-proton collision data
delivered by the Large Hadron Collider and recorded with the
ATLAS detector. Observations are consistent with the
Standard Model expectations and limits are set in
R-parity-conserving phenomenological Minimal Supersymmetric
Standard Models and in simplified supersymmetric models,
significantly extending previous results. For simplified
supersymmetric models of direct chargino (∼X±1) and
next-to-lightest neutralino (X∼02) production with decays
to lightest neutralino (∼X01) via either all three
generations of sleptons, staus only, gauge bosons, or Higgs
bosons, ∼X± 1 and ∼X02 masses are excluded up to
700GeV, 380GeV, 345GeV, or 148GeV respectively, for a
massless ∼X01.},
Doi = {10.1007/JHEP04(2014)169},
Key = {fds308281}
}
@article{fds336457,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Search for direct production of charginos, neutralinos and
sleptons in final states with two leptons and missing
transverse momentum in pp collisions at √s = 8TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {5},
Pages = {1-51},
Publisher = {Springer Nature},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2014)071},
Abstract = {Searches for the electroweak production of charginos,
neutralinos and sleptons in final states characterized by
the presence of two leptons (electrons and muons) and
missing transverse momentum are performed using 20.3 fb-1of
proton-proton collision data at √s = 8TeV recorded with
the ATLAS experiment at the Large Hadron Collider. No
significant excess beyond Standard Model expectations is
observed. Limits are set on the masses of the lightest
chargino, next-to-lightest neutralino and sleptons for
different lightest-neutralino mass hypotheses in simplified
models. Results are also interpreted in various scenarios of
the phenomenological Minimal Supersymmetric Standard
Model.},
Doi = {10.1007/JHEP05(2014)071},
Key = {fds336457}
}
@article{fds365429,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abulaiti, Y and Abreu, H and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Bella, LA and Arabidze, G},
Title = {Search for direct production of electroweakinos in final
states with one lepton, missing transverse momentum and a
Higgs boson decaying into two b-jets in pp collisions at
√s=13 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {8},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8050-3},
Abstract = {The results of a search for electroweakino pair production
pp→χ~1±χ~20 in which the chargino (χ~1±) decays into
a W boson and the lightest neutralino (χ~10), while the
heavier neutralino (χ~20) decays into the Standard Model
125 GeV Higgs boson and a second χ~10 are presented. The
signal selection requires a pair of b-tagged jets consistent
with those from a Higgs boson decay, and either an electron
or a muon from the W boson decay, together with missing
transverse momentum from the corresponding neutrino and the
stable neutralinos. The analysis is based on data
corresponding to 139 fb - 1 of s=13 TeV pp collisions
provided by the Large Hadron Collider and recorded by the
ATLAS detector. No statistically significant evidence of an
excess of events above the Standard Model expectation is
found. Limits are set on the direct production of the
electroweakinos in simplified models, assuming pure wino
cross-sections. Masses of χ~1±/χ~20 up to 740 GeV are
excluded at 95% confidence level for a massless
χ~10.},
Doi = {10.1140/epjc/s10052-020-8050-3},
Key = {fds365429}
}
@article{fds308310,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou-Zeid, OS and Abramowicz, H and Abreu, H and Kuday, S and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Chekanov, S and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov, VV and Dos Santos,
SPA and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Anulli,
F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Search for direct third-generation squark pair production in
final states with missing transverse momentum and two b-jets
in √s = 8 TeV pp collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {10},
Publisher = {Springer Nature},
Year = {2013},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP10(2013)189},
Abstract = {The results of a search for pair production of
supersymmetric partners of the Standard Model
third-generation quarks are reported. This search uses 20.1
fb−1 of pp collisions at √s = 8TeV collected by the
ATLAS experiment at the Large Hadron Collider. The lightest
bottom and top squarks (b1 and t1 respectively) are searched
for in a final state with large missing transverse momentum
and two jets identified as originating from b-quarks. No
excess of events above the expected level of Standard Model
background is found. The results are used to set upper
limits on the visible cross section for processes beyond the
Standard Model. Exclusion limits at the 95% confidence level
on the masses of the third-generation squarks are derived in
phenomenological supersymmetric R-parityconserving models in
which either the bottom or the top squark is the lightest
squark. The b1 is assumed to decay via b1 → bχ01 and the
t1 via t1 → bχ±1, with undetectable products of the
subsequent decay of the χ±1 due to the small mass
splitting between the χ±1 and the χ01.},
Doi = {10.1007/JHEP10(2013)189},
Key = {fds308310}
}
@article{fds321356,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Guimarães da Costa and JB and Bartoldus, R and Barton,
AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black,
CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Cameron, D and Caminada, LM and Armadans, RC and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli,
R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens,
JC},
Title = {Search for direct top squark pair production in events with
a [Formula: see text] boson, [Formula: see text]-jets and
missing transverse momentum in [Formula: see text] TeV
[Formula: see text] collisions with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {6},
Pages = {2883},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-2883-6},
Abstract = {A search is presented for direct top squark pair production
using events with at least two leptons including a
same-flavour opposite-sign pair with invariant mass
consistent with the [Formula: see text] boson mass, jets
tagged as originating from [Formula: see text]-quarks and
missing transverse momentum. The analysis is performed with
proton-proton collision data at [Formula: see text]
collected with the ATLAS detector at the LHC in 2012
corresponding to an integrated luminosity of
20.3 fb[Formula: see text]. No excess beyond the Standard
Model expectation is observed. Interpretations of the
results are provided in models based on the direct pair
production of the heavier top squark state ([Formula: see
text]) followed by the decay to the lighter top squark state
([Formula: see text]) via [Formula: see text], and for
[Formula: see text] pair production in natural
gauge-mediated supersymmetry breaking scenarios where the
neutralino ([Formula: see text]) is the next-to-lightest
supersymmetric particle and decays producing a [Formula: see
text] boson and a gravitino ([Formula: see text]) via the
[Formula: see text] process.},
Doi = {10.1140/epjc/s10052-014-2883-6},
Key = {fds321356}
}
@article{fds321348,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Search for direct top-squark pair production in final states
with two leptons in pp collisions at √s = 8 TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {6},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP06(2014)124},
Abstract = {A search is presented for direct top-squark pair production
in final states with two leptons (electrons or muons) of
opposite charge using 20.3 fb -1 of pp collision data at
√s = 8 TeV, collected by the ATLAS experiment at the Large
Hadron Collider in 2012. No excess over the Standard Model
expectation is found. The results are interpreted under the
separate assumptions (i) that the top squark decays to a
b-quark in addition to an on-shell chargino whose decay
occurs via a real or virtual W boson, or (ii) that the top
squark decays to a t-quark and the lightest neutralino. A
top squark with a mass between 150 GeV and 445 GeV decaying
to a b-quark and an on-shell chargino is excluded at 95%
confidence level for a top squark mass equal to the chargino
mass plus 10 GeV, in the case of a 1 GeV lightest
neutralino. Top squarks with masses between 215 (90) GeV and
530 (170) GeV decaying to an on-shell (off-shell) t-quark
and a neutralino are excluded at 95% confidence level for a
1 GeV neutralino. [Figure not available: see fulltext.] ©
2014 The Author(s).},
Doi = {10.1007/JHEP06(2014)124},
Key = {fds321348}
}
@article{fds375925,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
M and Bouquet, R and Marchiori, G and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
Gemmeren, P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Cui,
Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Unal, M and Webb, AF and Huseynov, N and Agaras, MN and Bosman, M and Casado,
MP},
Title = {Search for displaced photons produced in exotic decays of
the Higgs boson using 13 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032016},
Abstract = {A search is performed for delayed and nonpointing photons
originating from the displaced decay of a neutral long-lived
particle (LLP). The analysis uses the full run 2 dataset of
proton-proton collisions delivered by the LHC at a
center-of-mass energy of Formula Presented between 2015 and
2018 and recorded by the ATLAS detector, corresponding to an
integrated luminosity of Formula Presented. The capabilities
of the ATLAS electromagnetic calorimeter are exploited to
precisely measure the arrival times and trajectories of
photons. The results are interpreted in a scenario where the
LLPs are pair produced in exotic decays of the 125 GeV Higgs
boson, and each LLP subsequently decays into a photon and a
particle that escapes direct detection, giving rise to
missing transverse momentum. No significant excess is
observed above the expectation due to Standard Model
background processes. The results are used to set upper
limits on the branching ratio of the exotic decay of the
Higgs boson. A model-independent limit is also set on the
production of photons with large values of displacement and
time delay.},
Doi = {10.1103/PhysRevD.108.032016},
Key = {fds375925}
}
@article{fds365396,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arguin, JF and Argyropoulos,
S},
Title = {Search for doubly and singly charged Higgs bosons decaying
into vector bosons in multi-lepton final states with the
ATLAS detector using proton-proton collisions at √s = 13
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {6},
Year = {2021},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2021)146},
Abstract = {A search for charged Higgs bosons decaying into W±W± or
W±Z bosons is performed, involving experimental signatures
with two leptons of the same charge, or three or four
leptons with a variety of charge combinations, missing
transverse momentum and jets. A data sample of proton-proton
collisions at a centre-of-mass energy of 13 TeV recorded
with the ATLAS detector at the Large Hadron Collider between
2015 and 2018 is used. The data correspond to a total
integrated luminosity of 139 fb−1. The search is guided by
a type-II seesaw model that extends the scalar sector of the
Standard Model with a scalar triplet, leading to a
phenomenology that includes doubly and singly charged Higgs
bosons. Two scenarios are explored, corresponding to the
pair production of doubly charged H±± bosons, or the
associated production of a doubly charged H±± boson and a
singly charged H± boson. No significant deviations from the
Standard Model predictions are observed. H±± bosons are
excluded at 95% confidence level up to 350 GeV and 230 GeV
for the pair and associated production modes, respectively.
[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP06(2021)146},
Key = {fds365396}
}
@article{fds375942,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei,
D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Search for doubly charged Higgs boson production in
multi-lepton final states using 139 fb - 1 of
proton–proton collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11578-9},
Abstract = {A search for pair production of doubly charged Higgs bosons
(H± ±), each decaying into a pair of prompt, isolated, and
highly energetic leptons with the same electric charge, is
presented. The search uses a proton–proton collision data
sample at a centre-of-mass energy of 13 TeV corresponding
to an integrated luminosity of 139 fb - 1 recorded by the
ATLAS detector during Run 2 of the Large Hadron Collider
(LHC). This analysis focuses on same-charge leptonic decays,
H±±→ℓ±ℓ′± where ℓ,ℓ′=e,μ,τ , in two-,
three-, and four-lepton channels, but only considers final
states which include electrons or muons. No evidence of a
signal is observed. Corresponding upper limits on the
production cross-section of a doubly charged Higgs boson are
derived, as a function of its mass m(H± ±) , at 95%
confidence level. Assuming that the branching ratios to each
of the possible leptonic final states are equal, B(H± ±→
e±e±) = B(H± ±→ e±μ±) = B(H± ±→ μ±μ±) =
B(H± ±→ e±τ±) = B(H± ±→ μ±τ±) = B(H± ±→
τ±τ±) = 1 / 6 , the observed (expected) lower limit on
the mass of a doubly charged Higgs boson is 1080 GeV
(1065 GeV) within the left-right symmetric type-II seesaw
model, which is the strongest limit to date produced by the
ATLAS Collaboration. Additionally, this paper provides the
first direct test of the Zee–Babu neutrino mass model at
the LHC, yielding an observed (expected) lower limit of
m(H± ±) = 900 GeV (880 GeV).},
Doi = {10.1140/epjc/s10052-023-11578-9},
Key = {fds375942}
}
@article{fds308368,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for doubly charged Higgs bosons in like-sign dilepton
final states at √s = 7 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {72},
Number = {12},
Publisher = {Springer Nature},
Year = {2012},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2244-2},
Abstract = {A search for doubly charged Higgs bosons decaying to pairs
of electrons and/or muons is presented. The search is
performed using a data sample corresponding to an integrated
luminosity of 4.7 fb−1of pp collisions at √s = 7 TeV
collected by the ATLAS detector at the LHC. Pairs of prompt,
isolated, high-pT leptons with the same electric charge
(e±e±, e±μ±, μ±μ±) are selected, and their
invariant mass distribution is searched for a narrow
resonance. No significant excess over Standard Model
background expectations is observed, and limits are placed
on the cross section times branching ratio for pair
production of doubly charged Higgs bosons. The masses of
doubly charged Higgs bosons are constrained depending on the
branching ratio into these leptonic final states. Assuming
pair production, coupling to left-handed fermions, and a
branching ratio of 100% for each final state, masses below
409 GeV, 375 GeV, and 398 GeV are excluded for e±e±,
e±μ±, and μ±μ±, respectively.},
Doi = {10.1140/epjc/s10052-012-2244-2},
Key = {fds308368}
}
@article{fds344676,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch,
H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harr,
RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays,
C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans,
D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato,
Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu,
T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons,
L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller,
JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine,
A and Rappoccio, S and Ratnikov, F and Ray, H and Reichold, A and Reisert,
B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert,
K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz,
A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan,
A},
Title = {Search for electroweak single-top-quark production in pp̄
collisions at √s = 1.96 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {1},
Pages = {012005-1-012005-7},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.012005},
Abstract = {We report on a search for standard model t-channel and
s-channel single-top quark production in pp̄ collisions at
a center of mass energy of 1.96 TeV. We use a data sample
corresponding to 162 pb-1 recorded by the upgraded collider
detector at Fermilab. We find no significant evidence for
electroweak top quark production and set upper limits at the
95% confidence level on the production cross section,
consistent with the standard model: 10.1 pb for the
t-channel, 13.6 pb for the s-channel and 17.8 pb for the
combined cross section of t- and s-channel. © 2005 The
American Physical Society.},
Doi = {10.1103/PhysRevD.71.012005},
Key = {fds344676}
}
@article{fds308703,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann,
JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch,
H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson,
K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and da Costa, JG and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Karagoz Unel and M and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and Lecompte, T and Lee, J and Lee, SW and Lefevre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller,
JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, A-S and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
C and Pompos, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno,
M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna,
G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar,
S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A},
Title = {Search for excited and exotic electrons in the egamma decay
channel in pp collisions at sqrt[s] = 1.96
TeV.},
Journal = {Physical review letters},
Volume = {94},
Number = {10},
Pages = {101802},
Year = {2005},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.94.101802},
Abstract = {We present a search for excited and exotic electrons (e(*))
decaying to an electron and a photon, both with high
transverse momentum. We use 202 pb(-1) of data collected in
pp collisions at sqrt[s] = 1.96 TeV with the Collider
Detector at Fermilab II detector. No signal above standard
model expectation is seen for associated ee(*) production.
We discuss the e(*) sensitivity in the parameter space of
the excited electron mass M(e(*)) and the compositeness
energy scale Lambda. In the contact interaction model, we
exclude 132 GeV/c(2)<M(e(*))<879 GeV/c(2) for Lambda =
M(e(*)) at 95% confidence level (C.L.). In the
gauge-mediated model, we exclude 126 GeV/c(2) < M(e(*)) <
430 GeV/c(2) at 95% C.L. for the phenomenological coupling
f/Lambda approximately 10(-2) GeV-1.},
Doi = {10.1103/physrevlett.94.101802},
Key = {fds308703}
}
@article{fds308684,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri,
A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Ruzza, BD and Dionisi,
C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch, HJ and Furic, I and Gallinaro,
M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris, N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn,
SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer,
A and Heinemann, B and Heinrich, J and Herndon, M and Hidas, D and Hill,
CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden,
M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon,
EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato, Y and Kemp, Y and Kephart,
R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Mastrandrea, P and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh,
YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet,
M},
Title = {Search for excited and exotic muons in the μy decay channel
in pp - collisions at s=1.96 TeV},
Journal = {Physical Review Letters},
Volume = {97},
Number = {19},
Pages = {191802},
Year = {2006},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.97.191802},
Abstract = {We search for excited and exotic muon states * using an
integrated luminosity of 371pb-1 of pp collision data at
s=1.96TeV. We search for associated production of * followed
by the decay *. We compare the data to model predictions as
a function of the mass of the excited muon M *, the
compositeness energy scale , and the gauge coupling factor
f. No signal above the standard model expectation is
observed. We exclude 107<M *<853GeV/c2 for =M * in the
contact interaction model, and 100<M *<410GeV/c2 for
f/=10-2GeV-1 in the gauge-mediated model, both at the 95%
confidence level. © 2006 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.97.191802},
Key = {fds308684}
}
@article{fds308316,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Search for excited electrons and muons in √s=8 TeV
proton-proton collisions with the ATLAS detector},
Journal = {New Journal of Physics},
Volume = {15},
Number = {9},
Pages = {093011-093011},
Publisher = {IOP Publishing},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1088/1367-2630/15/9/093011},
Abstract = {The ATLAS detector at the Large Hadron Collider is used to
search for excited electrons and excited muons in the
channel pp → ℓℓ* → ℓℓγ, assuming that excited
leptons are produced via contact interactions. The analysis
is based on 13 fb-1 of pp collisions at a centre-of-mass
energy of 8 TeV. No evidence for excited leptons is found,
and a limit is set at the 95% credibility level on the cross
section times branching ratio as a function of the
excited-lepton mass mℓ*. For mℓ* 0.8 TeV, the respective
upper limits on σB(ℓ* → ℓγ) are 0.75 and 0.90 fb for
the e* and μ* searches. Limits on σB are converted into
lower bounds on the compositeness scale Λ. In the special
case where Λ = m ℓ*, excited-electron and excited-muon
masses below 2.2 TeV are excluded. © CERN
2013.},
Doi = {10.1088/1367-2630/15/9/093011},
Key = {fds308316}
}
@article{fds308618,
Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Behari,
S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carrillo, S and Carlsmith, D and Caron, B and Carosi, R and Carron,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Daronco, S and Datta, M and D'Auria, S and Davies, T and Dagenhart, D and de Barbaro, P and De
Cecco, S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Dörr,
C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron,
J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani,
M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson,
C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl,
D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marginean,
R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel,
P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles,
J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher,
G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore,
R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee,
A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov,
A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar,
S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet,
M},
Title = {Search for exclusive gammagamma production in Hadron-Hadron
collisions.},
Journal = {Physical review letters},
Volume = {99},
Number = {24},
Pages = {242002},
Year = {2007},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.99.242002},
Abstract = {We have searched for exclusive gammagamma production in
proton-antiproton collisions at sqrt[s]=1.96 TeV, using 532
pb(-1) of integrated luminosity taken by the run II Collider
Detector at Fermilab. The event signature requires two
electromagnetic showers, each with transverse energy E(T)>5
GeV and pseudorapidity |eta|<1.0, with no other particles
detected in the event. Three candidate events are observed.
We discuss the consistency of the three events with
gammagamma, pi(0)pi(0), or eta eta production. The
probability that other processes fluctuate to >or=3 events
is 1.7x10(-4). An upper limit on the cross section of pp-->p
+ gammagamma + p production is set at 410 fb with 95%
confidence level.},
Doi = {10.1103/physrevlett.99.242002},
Key = {fds308618}
}
@article{fds375885,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Search for exclusive Higgs and Z boson decays to ωγ and
Higgs boson decays to K⁎γ with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {847},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138292},
Abstract = {Searches for the exclusive decays of the Higgs boson to an
ω meson and a photon or a K⁎ meson and a photon can probe
flavour-conserving and flavour-violating Higgs boson
couplings to light quarks, respectively. Searches for these
decays, along with the analogous Z boson decay to an ω
meson and a photon, are performed with a pp collision data
sample corresponding to integrated luminosities of up to 134
fb−1 collected at s=13 TeV with the ATLAS detector at the
CERN Large Hadron Collider. The obtained 95%
confidence-level upper limits on the respective branching
fractions are B(H→ωγ)<5.5×10−4, B(H→K⁎γ)<2.2×10−4
and B(Z→ωγ)<3.9×10−6. The limits for H→ωγ and
Z→ωγ are 370 times and 140 times the Standard Model
expected values, respectively. The result for Z→ωγ
corresponds to a two-orders-of-magnitude improvement over
the limit obtained by the DELPHI experiment at
LEP.},
Doi = {10.1016/j.physletb.2023.138292},
Key = {fds375885}
}
@article{fds308547,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi,
F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell,
M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Di Canto and A and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Garosi, P and Genser, K and Gerberich,
H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee,
SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sinervo,
P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M},
Title = {Search for exclusive Z-boson production and observation of
high-mass pp[over ]-->pgammagammap[over ]-->pl;{+}l;{-}p[over
] events in pp[over ] collisions at sqrt[s]=1.96
TeV.},
Journal = {Physical review letters},
Volume = {102},
Number = {22},
Pages = {222002},
Year = {2009},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.102.222002},
Abstract = {This Letter presents a search for exclusive Z boson
production in proton-antiproton collisions at sqrt[s]=1.96
TeV, using the CDF II detector. No exclusive Z-->l;{+}l;{-}
candidates are observed and the first upper limit on the
exclusive Z cross section in hadron collisions is found to
be sigma_{excl}(Z)<0.96 pb at 95% confidence level. In
addition, eight candidate exclusive dilepton events from the
process pp[over ]-->pgammagammap[over ]-->pl;{+}l;{-}p[over
] are observed, and a measurement of the cross section for
M_{ll}>40 GeV/c;{2} and |eta_{l}|<4 is found to be
sigma=0.24_{-0.10};{+0.13} pb, which is consistent with the
standard model prediction.},
Doi = {10.1103/physrevlett.102.222002},
Key = {fds308547}
}
@article{fds308642,
Author = {Abulencia, and A, and others},
Title = {Search for Exotic $S=-2$ Baryons in $p\bar{p}$ Collisions at
$\sqrt{s}=1.96\,TeV$},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {3},
Pages = {032003},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.032003},
Abstract = {A search for a manifestly exotic S=-2 baryon state decaying
to Xi-pi-, and its neutral partner decaying to Xi-pi+, has
been performed using 220 pb-1 of p[overline p] collisions at
sqrt(s)=1.96 TeV collected by the Collider Detector at
Fermilab. The Xi- trajectories were measured in a silicon
tracker before their decay, resulting in a sample with low
background and excellent position resolution. No evidence
was found for S=-2 pentaquark candidates in the invariant
mass range of 1600--2100 MeV/c2. Upper limits on the product
of pentaquark production cross section times its branching
fraction to Xi-pi+,-, relative to the cross section of the
well-established Xi(1530) resonance, are presented for
neutral and doubly negative candidates with pT>2 GeV/c and
|y|},
Doi = {10.1103/PhysRevD.75.032003},
Key = {fds308642}
}
@article{fds365363,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala,
J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada
Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF},
Title = {Search for exotic decays of the Higgs boson into b b¯ and
missing transverse momentum in pp collisions at √s = 13
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2022},
Number = {1},
Year = {2022},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2022)063},
Abstract = {A search for the exotic decay of the Higgs boson (H) into a
bb¯ resonance plus missing transverse momentum is
described. The search is performed with the ATLAS detector
at the Large Hadron Collider using 139 fb−1 of pp
collisions at s = 13 TeV. The search targets events from ZH
production in an NMSSM scenario where H → χ~20χ~10, with
χ~20→aχ~10, where a is a light pseudoscalar Higgs boson
and χ~1,20 are the two lightest neutralinos. The decay of
the a boson into a pair of b-quarks results in a peak in the
dijet invariant mass distribution. The final-state signature
consists of two leptons, two or more jets, at least one of
which is identified as originating from a b-quark, and
missing transverse momentum. Observations are consistent
with Standard Model expectations and upper limits are set on
the product of cross section times branching ratio for a
three-dimensional scan of the masses of the χ~20, χ~10 and
a boson. [Figure not available: see fulltext.]},
Doi = {10.1007/JHEP01(2022)063},
Key = {fds365363}
}
@article{fds365375,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling, JH},
Title = {Search for exotic decays of the Higgs boson into long-lived
particles in pp collisions at √s = 13 TeV using displaced
vertices in the ATLAS inner detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2021)229},
Abstract = {A novel search for exotic decays of the Higgs boson into
pairs of long-lived neutral particles, each decaying into a
bottom quark pair, is performed using 139 fb−1 of s = 13
TeV proton-proton collision data collected with the ATLAS
detector at the LHC. Events consistent with the production
of a Higgs boson in association with a leptonically decaying
Z boson are analysed. Long-lived particle (LLP) decays are
reconstructed from inner-detector tracks as displaced
vertices with high mass and track multiplicity relative to
Standard Model processes. The analysis selection requires
the presence of at least two displaced vertices, effectively
suppressing Standard Model backgrounds. The residual
background contribution is estimated using a data-driven
technique. No excess over Standard Model predictions is
observed, and upper limits are set on the branching ratio of
the Higgs boson to LLPs. Branching ratios above 10% are
excluded at 95% confidence level for LLP mean proper
lifetimes cτ as small as 4 mm and as large as 100 mm. For
LLP masses below 40 GeV, these results represent the most
stringent constraint in this lifetime regime. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP11(2021)229},
Key = {fds365375}
}
@article{fds308849,
Author = {al, FAE},
Title = {Search for first generation leptoquark pair production in
p(p)over-bar collisions at root s=1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {79},
Number = {22},
Pages = {4327-4332},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.4327},
Abstract = {We present the results of a search for first generation
scalar leptoquarks pairs (S1S®1) in 110 ± 7 pb−1 of data
collected by the Collider Detector at Fermilab. We assume
both leptoquarks decay to an electron and a quark. Three
candidate events, with masses below 140 GeV/c2 and
consistent with background expectations, are observed. We
obtain a 95% confidence level upper limit on the production
cross section as a function of the leptoquark mass. Using a
next-to-leading order calculation of S1S®1 production, we
exclude scalar leptoquarks with mass less than 213GeV/c2 at
95% C.L. for a branching ratio into eq equal to 1. © 1997
American Physical Society.},
Doi = {10.1103/PhysRevLett.79.4327},
Key = {fds308849}
}
@article{fds308683,
Author = {Acosta, and D, and others},
Title = {Search for first-generation scalar leptoquarks in pp-bar
collisions at sqrt[s]=1.96 TeV},
Journal = {Phys. Rev.},
Volume = {D72},
Number = {5},
Pages = {051107},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.73.051102},
Abstract = {Results on a search for pair production of second-generation
scalar leptoquark in pp̄ collisions at s=1.96TeV are
reported. The data analyzed were collected by the CDF
detector during the 2002-2003 Tevatron Run II and correspond
to an integrated luminosity of 198pb-1. Leptoquarks (LQ) are
sought through their decay into (charged) leptons and
quarks, with final state signatures represented by two muons
and jets and one muon, large transverse missing energy and
jets. We observe no evidence for LQ production and derive
95% C.L. upper limits on the LQ production cross sections as
well as lower limits on their mass as a function of β,
where β is the branching fraction for LQ→μq. © 2006 The
American Physical Society.},
Doi = {10.1103/PhysRevD.73.051102},
Key = {fds308683}
}
@article{fds308883,
Author = {al, FAE},
Title = {Search for flavor-changing neutral current B meson decays in
p(p)over-bar collisions at root s=1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {76},
Number = {25},
Pages = {4675-4680},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevLett.76.4675},
Abstract = {We report on a search for the flavor-changing neutral
current decays B0d, s→μ+μ−, B+→μ+μ−K+, and
B0→μ+μ−K*0 using data from pp- collisions at s = 1.8
TeV, collected with the Collider Detector at Fermilab during
the 1992-1993 running period. We find no indication of such
decays, and we set the following 90% confidence level upper
limits on branching ratios: B\(B0→μ+μ−\)<1.6×10−6,
B(B0s→μ+μ−\)<8.4×10−6, B\(B+→μ+μ−K+\)<1.0×10−5,
and B\(B0→μ+μ−K*0\)<2.5×10−5. © 1996 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.76.4675},
Key = {fds308883}
}
@article{fds375926,
Author = {Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Sharma, AS and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Belfkir, M and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Franco,
L and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo Martinez and N and Portales, L and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem,
L and Wingerter-Seez, I and Abulaiti, Y and Bhopatkar, VS and Chekanov,
S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love,
J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
Gemmeren, P and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Delitzsch, CM and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Little, JD and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas,
L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Gazis, EN and Gkountoumis, P and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Zacharis, G and Andeen, T and Burton, CD and Choi, K and Nikiforou, N and Onyisi, PUE and Panchal, DK and Roy, A and Unal, M and Webb, AF and Adiguzel,
A},
Title = {Search for flavor-changing neutral-current couplings between
the top quark and the Z boson with proton-proton
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032019},
Abstract = {A search for flavor-changing neutral-current couplings
between a top quark, an up or charm quark, and a Formula
Presented boson is presented, using proton-proton collision
data at Formula Presented collected by the ATLAS detector at
the Large Hadron Collider. The analyzed data set corresponds
to an integrated luminosity of Formula Presented. The search
targets both single-top-quark events produced as Formula
Presented (with Formula Presented, Formula Presented) and
top-quark-pair events, with one top quark decaying through
the Formula Presented channel. The analysis considers events
with three leptons (electrons or muons), a Formula
Presented-tagged jet, possible additional jets, and missing
transverse momentum. The data are found to be consistent
with the background-only hypothesis and 95% confidence-level
limits on the Formula Presented branching ratios, assuming
only tensor operators of the Standard Model effective field
theory framework contribute to the Formula Presented
vertices. These are Formula Presented (Formula Presented)
for Formula Presented (Formula Presented) for a left-handed
Formula Presented coupling, and Formula Presented (Formula
Presented) in the case of a right-handed coupling. These
results are interpreted as 95% CL upper limits on the
strength of the corresponding couplings, yielding limits for
Formula Presented and Formula Presented (Formula Presented
and Formula Presented) of 0.15 (0.16), and limits for
Formula Presented and Formula Presented (Formula Presented
and Formula Presented) of 0.22 (0.21), assuming a
new-physics energy scale Formula Presented of 1
TeV.},
Doi = {10.1103/PhysRevD.108.032019},
Key = {fds375926}
}
@article{fds321214,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for flavour-changing neutral current top quark decays
t → Hq in pp collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {12},
Pages = {1-65},
Publisher = {Springer Nature},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2015)061},
Abstract = {Abstract: A search for flavour-changing neutral current
decays of a top quark to an uptype quark (q = u, c) and the
Standard Model Higgs boson, where the Higgs boson decays
to(Formula Presented.), is presented. The analysis searches
for top quark pair events in which one top quark decays to
Wb, with the W boson decaying leptonically, and the other
top quark decays to Hq. The search is based on pp collisions
at (Formula Presented.) TeV recorded in 2012 with the ATLAS
detector at the CERN Large Hadron Collider and uses an
integrated luminosity of 20.3 fb−1. Data are analysed in
the lepton-plus-jets final state, characterised by an
isolated electron or muon and at least four jets. The search
exploits the high multiplicity of b-quark jets
characteristic of signal events, and employs a likelihood
discriminant that uses the kinematic differences between the
signal and the background, which is dominated by (Formula
Presented.) decays. No significant excess of events above
the background expectation is found, and observed (expected)
95% CL upper limits of 0.56% (0.42%) and 0.61% (0.64%) are
derived for the t → Hc and t → Hu branching ratios
respectively. The combination of this search with other
ATLAS searches in the H → γγ and H → WW*, ττ decay
modes significantly improves the sensitivity, yielding
observed (expected) 95% CL upper limits on the t → Hc and
t → Hu branching ratios of 0.46% (0.25%) and 0.45% (0.29%)
respectively. The corresponding combined observed (expected)
upper limits on the |λtcH| and |λtuH| couplings are 0.13
(0.10) and 0.13 (0.10) respectively. These are the most
restrictive direct bounds on tqH interactions measured so
far.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP12(2015)061},
Key = {fds321214}
}
@article{fds375933,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA},
Title = {Search for flavour-changing neutral-current couplings
between the top quark and the photon with the ATLAS detector
at s=13 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {842},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1016/j.physletb.2022.137379},
Abstract = {This letter documents a search for flavour-changing neutral
currents (FCNCs), which are strongly suppressed in the
Standard Model, in events with a photon and a top quark with
the ATLAS detector. The analysis uses data collected in pp
collisions at s=13 TeV during Run 2 of the LHC,
corresponding to an integrated luminosity of 139 fb−1.
Both FCNC top-quark production and decay are considered. The
final state consists of a charged lepton, missing transverse
momentum, a b-tagged jet, one high-momentum photon and
possibly additional jets. A multiclass deep neural network
is used to classify events either as signal in one of the
two categories, FCNC production or decay, or as background.
No significant excess of events over the background
prediction is observed and 95% CL upper limits are placed on
the strength of left- and right-handed FCNC interactions.
The 95% CL bounds on the branching fractions for the FCNC
top-quark decays, estimated (expected) from both top-quark
production and decay, are B(t→uγ)<0.85(0.88−0.25+0.37)×10−5
and B(t→cγ)<4.2(3.40−0.95+1.35)×10−5 for a
left-handed tqγ coupling, and B(t→uγ)<1.2(1.20−0.33+0.50)×10−5
and B(t→cγ)<4.5(3.70−1.03+1.47)×10−5 for a
right-handed coupling.},
Doi = {10.1016/j.physletb.2022.137379},
Key = {fds375933}
}
@article{fds365357,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C},
Title = {Search for flavour-changing neutral-current interactions of
a top quark and a gluon in pp collisions at √s=13 TeV with
the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {4},
Year = {2022},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10182-7},
Abstract = {A search is presented for the production of a single top
quark via left-handed flavour-changing neutral-current
(FCNC) interactions of a top quark, a gluon and an up or
charm quark. Two production processes are considered: u+
g→ t and c+ g→ t. The analysis is based on
proton–proton collision data taken at a centre-of-mass
energy of 13 TeV with the ATLAS detector at the LHC. The
data set corresponds to an integrated luminosity of 139 fb-
1. Events with exactly one electron or muon, exactly one
b-tagged jet and missing transverse momentum are selected,
resembling the decay products of a singly produced top
quark. Neural networks based on kinematic variables
differentiate between events from the two signal processes
and events from background processes. The measured data are
consistent with the background-only hypothesis, and limits
are set on the production cross-sections of the signal
processes: σ(u+g→t)×B(t→Wb)×B(W→ℓν)<3.0pb and
σ(c+g→t)×B(t→Wb)×B(W→ℓν)<4.7pb at the 95%
confidence level, with B(W→ ℓν) = 0.325 being the sum
of branching ratios of all three leptonic decay modes of the
W boson. Based on the framework of an effective field
theory, the cross-section limits are translated into limits
on the strengths of the tug and tcg couplings occurring in
the theory: |CuGut|/Λ2<0.057TeV- 2 and |CuGct|/Λ2<0.14TeV-
2. These bounds correspond to limits on the branching ratios
of FCNC-induced top-quark decays: B(t→ u+ g) < 0.61 × 10
- 4 and B(t→ c+ g) < 3.7 × 10 - 4.},
Doi = {10.1140/epjc/s10052-022-10182-7},
Key = {fds365357}
}
@article{fds308873,
Author = {al, FAE},
Title = {Search for gluino and squark cascade decays at the Fermilab
tevatron collider},
Journal = {Phys. Rev. Lett.},
Volume = {76},
Number = {12},
Pages = {2006-2010},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevLett.76.2006},
Abstract = {We report on a search for supersymmetry using dilepton
events which complements the classic missing ET plus
multijet analyses. Using 19pb-1 of pp collisions at √s =
1.8TeV recorded with the Collider Detector at Fermilab we
have searched for squarks and gluinos decaying into
charginos and producing events with two leptons. We observe
one candidate event. In comparison, the expected number of
background events from standard model processes is
2.39±0.63(stat)+0.77-0.42(syst). Hence we set limits on
gluino and squark production based on predictions from the
supergravity inspired minimal supersymmetric extension of
the standard model. © 1996 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.76.2006},
Key = {fds308873}
}
@article{fds308525,
Author = {Aaltonen, T and others},
Title = {Search for Gluino-Mediated Bottom Squark Production in
p[overline p] Collisions at sqrt(s) = 1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {22},
Pages = {221801},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.221801},
Abstract = {We report on a search for the supersymmetric partner of the
bottom quark produced from gluino decays in data from 2.5
fb;{-1} of integrated luminosity collected by the Collider
Detector at Fermilab at sqrt[s]=1.96 TeV. Candidate events
are selected requiring two or more jets and large missing
transverse energy. At least two of the jets are required to
be tagged as originating from a b quark to enhance the
sensitivity. The results are in good agreement with the
prediction of the standard model processes, giving no
evidence for gluino decay to bottom squarks. This result
constrains the gluino-pair-production cross section to be
less than 40 fb at 95% credibility level for a gluino mass
of 350 GeV/c;{2}.},
Doi = {10.1103/physrevlett.102.221801},
Key = {fds308525}
}
@article{fds330936,
Author = {al, TAE},
Title = {Search for Gluinos and Scalar Quarks in pp Collisionsat
$\sqrt{s} = 1.8 TeV Using the Missing Energy plus Multijets
Signature},
Journal = {Physical Review Letters},
Volume = {88},
Number = {4},
Pages = {041801},
Year = {2002},
url = {http://dx.doi.org/10.1103/physrevlett.88.041801},
Abstract = {We have performed a search for gluinos (g) and scalar quarks
(q) in a data sample of 84 pb(-1) of pp collisions at square
root[s] = 1.8 TeV, recorded by the Collider Detector at
Fermilab. We investigate the final state of large missing
transverse energy and three or more jets, a characteristic
signature in R-parity-conserving supersymmetric models. The
analysis has been performed "blind," in that the inspection
of the signal region is made only after the predictions from
standard model backgrounds have been calculated. Comparing
the data with predictions of constrained supersymmetric
models, we exclude gluino masses below 195 GeV/c2 (95%
C.L.), independent of the squark mass. For the case m(q)
approximately m(g), gluino masses below 300 GeV/c2 are
excluded.},
Doi = {10.1103/physrevlett.88.041801},
Key = {fds330936}
}
@article{fds308860,
Author = {al, FAE},
Title = {Search for gluinos and squarks at the Fermilab tevatron
collider},
Journal = {Phys. Rev. D},
Volume = {56},
Number = {3},
Pages = {R1357-R1362},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.56.R1357},
Abstract = {We report on a search for supersymmetric squark and gluino
particles in a data sample of 19 [Formula presented] of
[Formula presented] collisions at [Formula presented] TeV
recorded by the Collider Detector at Fermilab. We searched
for events containing jets plus appreciable missing
transverse energy [Formula presented] This signature is
indicative of pair production and subsequent decay of
squarks and/or gluinos. After all cuts, there are [Formula
presented] events with [Formula presented] GeV and three
jets, and [Formula presented] events with [Formula
presented] GeV and four jets. These numbers of events are
consistent with estimates of standard model processes plus
detector-induced background sources. The analysis yields
lower limits on gluino and squark masses, based on the
predictions from the mnimal supersymmetric extension of the
standard model. At the [Formula presented] confidence level,
we find gluino and squark mass limits up to 216 [Formula
presented] assuming equal gluino and squark masses, and
gluino mass limits up to [Formula presented] [Formula
presented] independent of squark mass. © 1997 The American
Physical Society.},
Doi = {10.1103/PhysRevD.56.R1357},
Key = {fds308860}
}
@article{fds321156,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner,
M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji,
W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin,
S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret,
MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini,
I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro,
NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas,
CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Search for gluinos in events with an isolated lepton, jets
and missing transverse momentum at [Formula: see text] = 13
Te V with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {10},
Pages = {565},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4397-x},
Abstract = {The results of a search for gluinos in final states with an
isolated electron or muon, multiple jets and large missing
transverse momentum using proton-proton collision data at a
centre-of-mass energy of [Formula: see text] are presented.
The dataset used was recorded in 2015 by the ATLAS
experiment at the Large Hadron Collider and corresponds to
an integrated luminosity of 3.2 fb[Formula: see text]. Six
signal selections are defined that best exploit the signal
characteristics. The data agree with the Standard Model
background expectation in all six signal selections, and the
largest deviation is a 2.1 standard deviation excess. The
results are interpreted in a simplified model where
pair-produced gluinos decay via the lightest chargino to the
lightest neutralino. In this model, gluinos are excluded up
to masses of approximately 1.6 Te V depending on the mass
spectrum of the simplified model, thus surpassing the limits
of previous searches.},
Doi = {10.1140/epjc/s10052-016-4397-x},
Key = {fds321156}
}
@article{fds308537,
Author = {Aaltonen, T and others},
Title = {Search for hadronic decays of W and Z bosons in photon
events in pp̅ collisions at sqrt[s] =1.96
TeV},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {5},
Pages = {052011},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.052011},
Abstract = {We report on a search for the process pp̅ →γ+W/Z with
W/Z→qq̅ in events containing two jets and a photon at the
center-of-mass energy sqrt[s]=1.96 TeV, using
184 pb-1 of data collected by the CDF II detector. A
neural network event selection has been developed to
optimize the rejection of the large QCD production
background; it is shown that this method gives a significant
improvement in both signal-to-noise ratio and signal
sensitivity, as compared with an event selection based on
conventional cuts. An upper limit is presented for the
γ+W/Z production cross section with the W and Z decaying
hadronically.},
Doi = {10.1103/PhysRevD.80.052011},
Key = {fds308537}
}
@article{fds308441,
Author = {Aaltonen, and T, and al, E},
Title = {Search for Heavy Bottomlike Quarks Decaying to an Electron
or Muon and Jets in $p\overline{p}$ Collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {14},
Pages = {141803},
Publisher = {American Physical Society},
Year = {2011},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.141803},
Abstract = {We report the most sensitive direct search for pair
production of fourth-generation bottomlike chiral quarks
(b') each decaying promptly to tW. We search for an excess
of events with an electron or muon, at least five jets (one
identified as due to a b or c quark), and an imbalance of
transverse momentum by using data from pp collisions
collected by the CDF II detector at Fermilab with an
integrated luminosity of 4.8 fb(-1). We observe events
consistent with background expectation, calculate upper
limits on the b' pair-production cross section (σ(bb'))
≲30 fb for m(b') > 375 GeV/c2), and exclude
m(b') < 372 GeV/c2 at 95% confidence level assuming a
100% branching ratio of b' to tW.},
Doi = {10.1103/PhysRevLett.106.141803},
Key = {fds308441}
}
@article{fds365420,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti,
C},
Title = {Search for heavy diboson resonances in semileptonic final
states in pp collisions at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {12},
Year = {2020},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08554-y},
Abstract = {This paper reports on a search for heavy resonances decaying
into WW, ZZ or WZ using proton–proton collision data at a
centre-of-mass energy of s=13 TeV. The data, corresponding
to an integrated luminosity of 139 fb 1, were recorded with
the ATLAS detector from 2015 to 2018 at the Large Hadron
Collider. The search is performed for final states in which
one W or Z boson decays leptonically, and the other W boson
or Z boson decays hadronically. The data are found to be
described well by expected backgrounds. Upper bounds on the
production cross sections of heavy scalar, vector or tensor
resonances are derived in the mass range 300–5000 GeV
within the context of Standard Model extensions with warped
extra dimensions or including a heavy vector triplet.
Production through gluon–gluon fusion, Drell–Yan or
vector-boson fusion are considered, depending on the assumed
model.},
Doi = {10.1140/epjc/s10052-020-08554-y},
Key = {fds365420}
}
@article{fds314181,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for heavy lepton resonances decaying to a Z boson and
a lepton in pp collisions at s√=8},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {9},
Pages = {1-38},
Publisher = {Springer Nature},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2015)108},
Abstract = {A search for heavy leptons decaying to a Z boson and an
electron or a muon is presented. The search is based on pp
collision data taken at (Formula presented.) = 8 TeV by the
ATLAS experiment at the CERN Large Hadron Collider,
corresponding to an integrated luminosity of 20.3 fb−1.
Three high-transverse-momentum electrons or muons are
selected, with two of them required to be consistent with
originating from a Z boson decay. No significant excess
above Standard Model background predictions is observed, and
95% confidence level limits on the production cross section
of high-mass trilepton resonances are derived. The results
are interpreted in the context of vector-like lepton and
type-III seesaw models. For the vector-like lepton model,
most heavy lepton mass values in the range 114–176 GeV are
excluded. For the type-III seesaw model, most mass values in
the range 100–468 GeV are excluded.},
Doi = {10.1007/JHEP09(2015)108},
Key = {fds314181}
}
@article{fds321160,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adersberger, M and Adomeit, S and Adye,
T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Search for heavy long-lived charged R-hadrons with the ATLAS
detector in 3.2 fb−1 of proton–proton
collision data at √s=13 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {760},
Pages = {647-665},
Publisher = {Elsevier BV},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2016.07.042},
Abstract = {A search for heavy long-lived charged R-hadrons is reported
using a data sample corresponding to 3.2 fb−1 of
proton–proton collisions at s=13 TeV collected by the
ATLAS experiment at the Large Hadron Collider at CERN. The
search is based on observables related to large ionisation
losses and slow propagation velocities, which are signatures
of heavy charged particles travelling significantly slower
than the speed of light. No significant deviations from the
expected background are observed. Upper limits at 95%
confidence level are provided on the production cross
section of long-lived R-hadrons in the mass range from 600
GeV to 2000 GeV and gluino, bottom and top squark masses are
excluded up to 1580 GeV, 805 GeV and 890 GeV,
respectively.},
Doi = {10.1016/j.physletb.2016.07.042},
Key = {fds321160}
}
@article{fds321304,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
C},
Title = {Search for heavy long-lived multi-charged particles in
pp collisions at [Formula: see text] TeV using the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {8},
Pages = {362},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3534-2},
Abstract = {A search for heavy long-lived multi-charged particles is
performed using the ATLAS detector at the LHC. Data
collected in 2012 at [Formula: see text] TeV from <i>pp</i>
collisions corresponding to an integrated luminosity of
20.3 fb[Formula: see text]are examined. Particles producing
anomalously high ionisation, consistent with long-lived
massive particles with electric charges from [Formula: see
text] to [Formula: see text] are searched for. No signal
candidate events are observed, and 95 % confidence level
cross-section upper limits are interpreted as lower mass
limits for a Drell-Yan production model. The mass limits
range between 660 and 785 GeV.},
Doi = {10.1140/epjc/s10052-015-3534-2},
Key = {fds321304}
}
@article{fds375886,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos,
KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Search for heavy long-lived multi-charged particles in the
full LHC Run 2 pp collision data at s=13 TeV using the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {847},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138316},
Abstract = {A search for heavy long-lived multi-charged particles is
performed using the ATLAS detector at the LHC. Data
collected in 2015–2018 at s=13 TeV from pp collisions
corresponding to an integrated luminosity of 139 fb−1 are
examined. Particles producing anomalously high ionization,
consistent with long-lived spin-½ massive particles with
electric charges from |q|=2e to |q|=7e are searched for. No
statistically significant evidence of such particles is
observed, and 95% confidence level cross-section upper
limits are calculated and interpreted as the lower mass
limits for a Drell–Yan plus photon-fusion production mode.
The least stringent limit, 1060 GeV, is obtained for |q|=2e
particles, and the most stringent one, 1600 GeV, is for
|q|=6e particles.},
Doi = {10.1016/j.physletb.2023.138316},
Key = {fds375886}
}
@article{fds316655,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold,
H},
Title = {Search for heavy Majorana neutrinos with the ATLAS detector
in pp collisions at √s = 8 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {7},
Publisher = {Springer Nature},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2015)162},
Abstract = {Abstract: A search for heavy Majorana neutrinos in events
containing a pair of high-pT leptons of the same charge and
high-pT jets is presented. The search uses 20.3 fb−1 of pp
collision data collected with the ATLAS detector at the CERN
Large Hadron Collider with a centre-of-mass energy of 221as
= 8 TeV. The data are found to be consistent with the
background-only hypothesis based on the Standard Model
expectation. In the context of a Type-I seesaw mechanism,
limits are set on the production cross-section times
branching ratio for production of heavy Majorana neutrinos
in the mass range between 100 and 500 GeV. The limits are
subsequently interpreted as limits on the mixing between the
heavy Majorana neutrinos and the Standard Model neutrinos.
In the context of a left-right symmetric model, limits on
the production cross-section times branching ratio are set
with respect to the masses of heavy Majorana neutrinos and
heavy gauge bosons WR and Z′.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP07(2015)162},
Key = {fds316655}
}
@article{fds375883,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Arcangeletti,
C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Tame,
ZPA and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Gupta, DB and Balasubramanian, R and Baldin,
EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas,
WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits,
M-S and Barklow, T and Baron, P and Moreno, DAB and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Navarro, LB and Barreiro, F and da
Costa, JBG and Barron, U and Teixeira, MGB and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Hurrell, LTB and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Kuutmann, EB and Berger, N and Bergmann, B and Beringer, J and Bernardi,
G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta,
P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Sola, JDB and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and de Renstrom, PAB and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Vazquez, CJB and Buzykaev, AR and Cabras, G and Urbán, SC and Caforio,
D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Toro, RC and Camarda, S and Munoz, DC and Camarri, P and Camerlingo, MT and Cameron,
D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Bret, MC and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson,
BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Argos, FC and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia,
EG and Castillo, FL and Garcia, LC and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Moursli, RCE and Cheu, E and Cheung, K and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi,
K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron,
ZH},
Title = {Search for heavy Majorana or Dirac neutrinos and
right-handed W gauge bosons in final states with charged
leptons and jets in pp collisions at $$\sqrt{s}=13$$ TeV
with the ATLAS detector},
Journal = {The European Physical Journal C},
Volume = {83},
Number = {12},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-12021-9},
Abstract = {<jats:title>Abstract</jats:title><jats:p>A search for heavy
right-handed Majorana or Dirac neutrinos
<jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
and heavy right-handed gauge bosons <jats:inline-formula><jats:alternatives><jats:tex-math>$$W_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>W</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
is performed in events with energetic electrons or muons,
with the same or opposite electric charge, and energetic
jets. The search is carried out separately for topologies of
clearly separated final-state products (“resolved”
channel) and topologies with boosted final states with
hadronic and/or leptonic products partially overlapping and
reconstructed as a large-radius jet (“boosted” channel).
The events are selected from <jats:italic>pp</jats:italic>
collision data at the LHC with an integrated luminosity of
139 fb<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{-1}$$</jats:tex-math>??
<mml:msup> <mml:mrow /> <mml:mrow> <mml:mo>-</mml:mo>
<mml:mn>1</mml:mn> </mml:mrow> </mml:msup>
</mml:math></jats:alternatives></jats:inline-formula>
collected by the ATLAS detector at <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sqrt{s}
= 13$$</jats:tex-math>?? <mml:mrow> <mml:msqrt>
<mml:mi>s</mml:mi> </mml:msqrt> <mml:mo>=</mml:mo>
<mml:mn>13</mml:mn> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> TeV.
No significant deviations from the Standard Model
predictions are observed. The results are interpreted within
the theoretical framework of a left-right symmetric model,
and lower limits are set on masses in the heavy right-handed
<jats:inline-formula><jats:alternatives><jats:tex-math>$$W_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>W</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
boson and <jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
plane. The excluded region extends to about
<jats:inline-formula><jats:alternatives><jats:tex-math>$$m(W_{\textrm{R}})
= 6.4$$</jats:tex-math>?? <mml:mrow> <mml:mi>m</mml:mi>
<mml:mo>(</mml:mo> <mml:msub> <mml:mi>W</mml:mi>
<mml:mtext>R</mml:mtext> </mml:msub> <mml:mo>)</mml:mo>
<mml:mo>=</mml:mo> <mml:mn>6.4</mml:mn> </mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula> TeV
for both Majorana and Dirac <jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
neutrinos at <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(N_{\textrm{R}})<1$$</jats:tex-math>??
<mml:mrow> <mml:mi>m</mml:mi> <mml:mo>(</mml:mo> <mml:msub>
<mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext> </mml:msub>
<mml:mo>)</mml:mo> <mml:mo><</mml:mo> <mml:mn>1</mml:mn>
</mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> TeV.
<jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
with masses of less than 3.5 (3.6) TeV are excluded in the
electron (muon) channel at <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(W_{\textrm{R}})=4.8$$</jats:tex-math>??
<mml:mrow> <mml:mi>m</mml:mi> <mml:mo>(</mml:mo> <mml:msub>
<mml:mi>W</mml:mi> <mml:mtext>R</mml:mtext> </mml:msub>
<mml:mo>)</mml:mo> <mml:mo>=</mml:mo> <mml:mn>4.8</mml:mn>
</mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> TeV
for the Majorana neutrinos, and limits of
<jats:inline-formula><jats:alternatives><jats:tex-math>$$m(N_{\textrm{R}})$$</jats:tex-math>??
<mml:mrow> <mml:mi>m</mml:mi> <mml:mo>(</mml:mo> <mml:msub>
<mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext> </mml:msub>
<mml:mo>)</mml:mo> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula>
up to 3.6 TeV for <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(W_{\textrm{R}})
= 5.2$$</jats:tex-math>?? <mml:mrow> <mml:mi>m</mml:mi>
<mml:mo>(</mml:mo> <mml:msub> <mml:mi>W</mml:mi>
<mml:mtext>R</mml:mtext> </mml:msub> <mml:mo>)</mml:mo>
<mml:mo>=</mml:mo> <mml:mn>5.2</mml:mn> </mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula>
(5.0) TeV in the electron (muon) channel are set for the
Dirac neutrinos. These constitute the most stringent
exclusion limits to date for the model considered.</jats:p>},
Doi = {10.1140/epjc/s10052-023-12021-9},
Key = {fds375883}
}
@article{fds308401,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
Title = {Search for heavy metastable particles decaying to jet pairs
in pp̄ collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012007},
Abstract = {A search is performed for heavy metastable particles that
decay into jet pairs with a macroscopic lifetime (cτ∼1cm)
in pp̄ collisions at √s=1.96TeV using data from the CDF
II detector at Fermilab corresponding to an integrated
luminosity of 3.2fb-1. To estimate the standard model
background, a data-driven approach is used.
Probability-density functions are constructed to model
secondary vertices from known processes. No statistically
significant excess is observed above the background. Limits
on the production cross section in a hidden valley benchmark
phenomenology are set for various Higgs boson masses as well
as metastable particle masses and lifetimes. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.85.012007},
Key = {fds308401}
}
@article{fds375930,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Austrup, VA and Avner, G and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari,
T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini,
G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
D and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
Kuutmann, E and Berger, N and Bergmann, B and Beringer, J and Berlendis,
S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes,
CJ and Bird, GA and Birman, M and Bisanz, T and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Brickwedde,
B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks,
WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko,
D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler,
JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez,
CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura,
P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet,
D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin,
E and Carrá, S and Carratta, G and Carter, JWS and Carter, TM and Casadei,
D and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A and Clark, PJ and Clavijo Columbie and JM and Clawson, SE and Clement, C and Clissa, L and Coadou, Y and Cobal,
M},
Title = {Search for Heavy Neutral Leptons in Decays of W Bosons Using
a Dilepton Displaced Vertex in sqrt[s]=13 TeV pp
Collisions with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {6},
Pages = {061803},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.131.061803},
Abstract = {A search for a long-lived, heavy neutral lepton (N) in
139 fb^{-1} of sqrt[s]=13 TeV pp collision data
collected by the ATLAS detector at the Large Hadron Collider
is reported. The N is produced via W→Nμ or W→Ne and
decays into two charged leptons and a neutrino, forming a
displaced vertex. The N mass is used to discriminate between
signal and background. No signal is observed, and limits are
set on the squared mixing parameters of the N with the
left-handed neutrino states for the N mass range
3 GeV<m_{N}<15 GeV. For the first time, limits are
given for both single-flavor and multiflavor mixing
scenarios motivated by neutrino flavor oscillation results
for both the normal and inverted neutrino-mass
hierarchies.},
Doi = {10.1103/physrevlett.131.061803},
Key = {fds375930}
}
@article{fds335595,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik,
Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
M and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee,
S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary,
O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JSB and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt,
A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, DC and Chan, SK and Chan,
WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, J and Chen, S and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard,
AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Clark, A},
Title = {Search for heavy particles decaying into top-quark pairs
using lepton-plus-jets events in proton-proton collisions at
s = 13 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {7},
Pages = {565},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5995-6},
Abstract = {A search for new heavy particles that decay into top-quark
pairs is performed using data collected from proton-proton
collisions at a centre-of-mass energy of 13 TeV by the
ATLAS detector at the Large Hadron Collider. The integrated
luminosity of the data sample is 36.1 fb - 1 . Events
consistent with top-quark pair production are selected by
requiring a single isolated charged lepton, missing
transverse momentum and jet activity compatible with a
hadronic top-quark decay. Jets identified as likely to
contain <i>b</i>-hadrons are required to reduce the
background from other Standard Model processes. The
invariant mass spectrum of the candidate top-quark pairs is
examined for local excesses above the background
expectation. No significant deviations from the Standard
Model predictions are found. Exclusion limits are set on the
production cross-section times branching ratio for
hypothetical Z ' bosons, Kaluza-Kein gluons and Kaluza-Klein
gravitons that decay into top-quark pairs.},
Doi = {10.1140/epjc/s10052-018-5995-6},
Key = {fds335595}
}
@article{fds365403,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Search for heavy resonances decaying into a pair of Z bosons
in the ℓ+ℓ-ℓ′
+ℓ′ - and ℓ+ℓ-νν¯
final states using 139 fb - 1 of proton–proton
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09013-y},
Abstract = {A search for heavy resonances decaying into a pair of Z
bosons leading to ℓ+ℓ-ℓ′ +ℓ′ - and
ℓ+ℓ-νν¯ final states, where ℓ stands for either an
electron or a muon, is presented. The search uses
proton–proton collision data at a centre-of-mass energy of
13 TeV collected from 2015 to 2018 that corresponds to the
integrated luminosity of 139 fb - 1 recorded by the ATLAS
detector during Run 2 of the Large Hadron Collider.
Different mass ranges spanning 200 GeV to 2000 GeV for the
hypothetical resonances are considered, depending on the
final state and model. In the absence of a significant
observed excess, the results are interpreted as upper limits
on the production cross section of a spin-0 or spin-2
resonance. The upper limits for the spin-0 resonance are
translated to exclusion contours in the context of Type-I
and Type-II two-Higgs-doublet models, and the limits for the
spin-2 resonance are used to constrain the Randall–Sundrum
model with an extra dimension giving rise to spin-2 graviton
excitations.},
Doi = {10.1140/epjc/s10052-021-09013-y},
Key = {fds365403}
}
@article{fds335600,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for heavy resonances decaying into a W or Z boson and
a Higgs boson in final states with leptons and b-jets in 36
fb−1 of √s=13 TeV pp collisions with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {3},
Publisher = {Springer Nature},
Year = {2018},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2018)174},
Abstract = {A search is conducted for new resonances decaying into a W
or Z boson and a 125 GeV Higgs boson in the νν¯ bb¯ ,
ℓ±νbb¯ , and ℓ+ℓ−bb¯ final states, where ℓ± =
e± or μ±, in pp collisions at s=13 TeV. The data used
correspond to a total integrated luminosity of 36.1 fb−1
collected with the ATLAS detector at the Large Hadron
Collider during the 2015 and 2016 data-taking periods. The
search is conducted by examining the reconstructed invariant
or transverse mass distributions of W h and Zh candidates
for evidence of a localised excess in the mass range of 220
GeV up to 5 TeV. No significant excess is observed and the
results are interpreted in terms of constraints on the
production cross-section times branching fraction of heavy
W′ and Z′ resonances in heavy-vector-triplet models and
the CP-odd scalar boson A in two-Higgs-doublet models. Upper
limits are placed at the 95% confidence level and range
between 9.0 × 10−4 pb and 7.3 × 10−1 pb depending on
the model and mass of the resonance.[Figure not available:
see fulltext.].},
Doi = {10.1007/JHEP03(2018)174},
Key = {fds335600}
}
@article{fds308624,
Author = {Abulencia, and A, and others},
Title = {Search for heavy, long-lived particles that decay to photons
at CDF II},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {12},
Pages = {121801},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.121801},
Abstract = {We present the first search for heavy, long-lived particles
that decay to photons at a hadron collider. We use a sample
of gamma+jet+missing transverse energy events in p[overline
p] collisions at sqrt(s)=1.96 TeV taken with the CDF II
detector. Candidate events are selected based on the arrival
time of the photon at the detector. Using an integrated
luminosity of 570 pb-1 of collision data, we observe 2
events, consistent with the background estimate of
1.3$\pm$0.7 events. While our search strategy does not rely
on model-specific dynamics, we set cross section limits in a
supersymmetric model with chi-tilde10-->gammaG-tilde and
place the world-best 95\% C.L. lower limit on the
chi-tilde10 mass of 101 GeV/c2 at tauchi-tilde[sub 1][sup
0]=5 ns.},
Doi = {10.1103/physrevlett.99.121801},
Key = {fds308624}
}
@article{fds321266,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
Title = {Search for Higgs and Z Boson Decays to J/ψγ and ϒ(nS)γ
with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {12},
Pages = {121801},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.114.121801},
Abstract = {A search for the decays of the Higgs and Z bosons to J/ψγ
and ϒ(nS)γ (n=1,2,3) is performed with pp collision data
samples corresponding to integrated luminosities of up to
20.3 fb^{-1} collected at sqrt[s]=8 TeV with the
ATLAS detector at the CERN Large Hadron Collider. No
significant excess of events is observed above expected
backgrounds and 95% C.L. upper limits are placed on the
branching fractions. In the J/ψγ final state the limits
are 1.5×10^{-3} and 2.6×10^{-6} for the Higgs and Z boson
decays, respectively, while in the ϒ(1S,2S,3S)γ final
states the limits are (1.3,1.9,1.3)×10^{-3} and
(3.4,6.5,5.4)×10^{-6}, respectively.},
Doi = {10.1103/physrevlett.114.121801},
Key = {fds321266}
}
@article{fds321161,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
J and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M},
Title = {Search for Higgs and Z Boson Decays to ϕγ with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {117},
Number = {11},
Pages = {111802},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.117.111802},
Abstract = {A search for the decays of the Higgs and Z bosons to a ϕ
meson and a photon is performed with a pp collision data
sample corresponding to an integrated luminosity of
2.7 fb^{-1} collected at sqrt[s]=13 TeV with the
ATLAS detector at the LHC. No significant excess of events
is observed above the background, and 95% confidence level
upper limits on the branching fractions of the Higgs and Z
boson decays to ϕγ of 1.4×10^{-3} and 8.3×10^{-6},
respectively, are obtained.},
Doi = {10.1103/physrevlett.117.111802},
Key = {fds321161}
}
@article{fds308272,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and A°kesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ},
Title = {Search for Higgs boson decays to a photon and a Z boson in
pp collisions at s=7 and 8 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {732},
Pages = {8-27},
Publisher = {Elsevier BV},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2014.03.015},
Abstract = {A search is reported for a neutral Higgs boson in the decay
channel H→Zγ, Z→ℓ +ℓ -(ℓ = e, μ), using 4.5
fb-1of pp collisions at s=7 TeV and 20.3 fb-1of pp
collisions at s=8 TeV, recorded by the ATLAS detector at the
CERN Large Hadron Collider. The observed distribution of the
invariant mass of the three final-state particles,mℓℓγ,
is consistent with the Standard Model hypothesis in the
investigated mass range of 120-150 GeV. For a Higgs boson
with a mass of 125.5 GeV, the observed upper limit at the
95% confidence level is 11 times the Standard Model
expectation. Upper limits are set on the cross section times
branching ratio of a neutral Higgs boson with mass in the
range 120-150 GeV between 0.13 and 0.5 pb for s=8 TeV at 95%
confidence level. © 2014.},
Doi = {10.1016/j.physletb.2014.03.015},
Key = {fds308272}
}
@article{fds335598,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for Higgs boson decays to beyond-the-Standard-Model
light bosons in four-lepton events with the ATLAS detector
at √s=13 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {6},
Publisher = {Springer Nature},
Year = {2018},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2018)166},
Abstract = {A search is conducted for a beyond-the-Standard-Model boson
using events where a Higgs boson with mass 125 GeV decays to
four leptons (ℓ = e or μ). This decay is presumed to
occur via an intermediate state which contains one or two
on-shell, promptly decaying bosons: H → ZX/XX → 4ℓ,
where X is a new vector boson Zd or pseudoscalar a with mass
between 1 and 60 GeV. The search uses pp collision data
collected with the ATLAS detector at the LHC with an
integrated luminosity of 36.1 fb−1 at a centre-of-mass
energy s=13 TeV. No significant excess of events above
Standard Model background predictions is observed;
therefore, upper limits at 95% confidence level are set on
modelindependent fiducial cross-sections, and on the Higgs
boson decay branching ratios to vector and pseudoscalar
bosons in two benchmark models.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP06(2018)166},
Key = {fds335598}
}
@article{fds375943,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Search for Higgs boson pair production in association with a
vector boson in pp collisions at √s=13TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11559-y},
Abstract = {This paper reports a search for Higgs boson pair (hh)
production in association with a vector boson (WorZ) using
139 fb - 1 of proton–proton collision data at s=13TeV
recorded with the ATLAS detector at the Large Hadron
Collider. The search is performed in final states in which
the vector boson decays leptonically (W→ℓν,Z→ℓℓ,νν
with ℓ= e, μ) and the Higgs bosons each decay into a pair
of b-quarks. It targets Vhh signals from both non-resonant
hh production, present in the Standard Model (SM), and
resonant hh production, as predicted in some SM extensions.
A 95% confidence-level upper limit of 183 (87) times the SM
cross-section is observed (expected) for non-resonant Vhh
production when assuming the kinematics are as expected in
the SM. Constraints are also placed on Higgs boson coupling
modifiers. For the resonant search, upper limits on the
production cross-sections are derived for two specific
models: one is the production of a vector boson along with a
neutral heavy scalar resonance H, in the mass range
260–1000 GeV, that decays into hh, and the other is the
production of a heavier neutral pseudoscalar resonance A
that decays into a Z boson and H boson, where the A boson
mass is 360–800 GeV and the H boson mass is
260–400 GeV. Constraints are also derived in the
parameter space of two-Higgs-doublet models.},
Doi = {10.1140/epjc/s10052-023-11559-y},
Key = {fds375943}
}
@article{fds321305,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH},
Title = {Search for Higgs boson pair production in the [Formula: see
text] final state from pp collisions at [Formula: see
text] TeVwith the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {9},
Pages = {412},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3628-x},
Abstract = {A search for Higgs boson pair production [Formula: see text]
is performed with 19.5 fb[Formula: see text] of
proton-proton collision data at [Formula: see text] TeV,
which were recorded by the ATLAS detector at the Large
Hadron Collider in 2012. The decay products of each Higgs
boson are reconstructed as a high-momentum [Formula: see
text] system with either a pair of small-radius jets or a
single large-radius jet, the latter exploiting jet
substructure techniques and associated <i>b</i>-tagged
track-jets. No evidence for resonant or non-resonant Higgs
boson pair production is observed. The data are interpreted
in the context of the Randall-Sundrum model with a warped
extra dimension as well as the two-Higgs-doublet model. An
upper limit on the cross-section for [Formula: see text] of
3.2 (2.3) fb is set for a Kaluza-Klein graviton [Formula:
see text] mass of 1.0 (1.5) TeV, at the 95 % confidence
level. The search for non-resonant Standard Model <i>hh</i>
production sets an observed 95 % confidence level upper
limit on the production cross-section [Formula: see text] of
202 fb, compared to a Standard Model prediction of
[Formula: see text] fb.},
Doi = {10.1140/epjc/s10052-015-3628-x},
Key = {fds321305}
}
@article{fds321267,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin,
M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, MF and Besson, N and Betancourt,
C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea,
V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov,
A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG},
Title = {Search for Higgs boson pair production in the γγbb[over
¯] final state using pp collision data at
sqrt[s]=8 TeV from the ATLAS detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {8},
Pages = {081802},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.114.081802},
Abstract = {Searches are performed for resonant and nonresonant Higgs
boson pair production in the γγbb[over ¯] final state
using 20 fb^{-1} of proton-proton collisions at a
center-of-mass energy of 8 TeV recorded with the ATLAS
detector at the CERN Large Hadron Collider. A 95% confidence
level upper limit on the cross section times branching ratio
of nonresonant production is set at 2.2 pb, while the
expected limit is 1.0 pb. The difference derives from a
modest excess of events, corresponding to 2.4 standard
deviations from the background-only hypothesis. The limit
observed in the search for a narrow X→hh resonance ranges
between 0.7 and 3.5 pb as a function of the resonance
mass.},
Doi = {10.1103/physrevlett.114.081802},
Key = {fds321267}
}
@article{fds365411,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin,
JF},
Title = {Search for Higgs boson production in association with a
high-energy photon via vector-boson fusion with decay into
bottom quark pairs at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {3},
Year = {2021},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2021)268},
Abstract = {A search is presented for the production of the Standard
Model Higgs boson in association with a high-energy photon.
With a focus on the vector-boson fusion process and the
dominant Higgs boson decay into b-quark pairs, the search
benefits from a large reduction of multijet background
compared to more inclusive searches. Results are reported
from the analysis of 132 fb−1 of pp collision data at s =
13 TeV collected with the ATLAS detector at the LHC. The
measured Higgs boson signal yield in this final-state
signature is 1.3 ± 1.0 times the Standard Model prediction.
The observed significance of the Higgs boson signal above
the background is 1.3 standard deviations, compared to an
expected significance of 1.0 standard deviations. [Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP03(2021)268},
Key = {fds365411}
}
@article{fds43833,
Author = {M. C. Kruse and W. Yao, and D. Acosta et al. (CDF
Collaboration)},
Title = {Search for Higgs Bosons Decaying into $b\bar{b}$ and
Produced in Association with a Vector Boson in $p\bar{p}$
Collisions at $\sqrt{s} = 1.8$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {95},
Number = {051801},
Year = {2005},
url = {http://arxiv.org/pdf/hep-ex/0503039},
Abstract = {http://arxiv.org/abs/hep-ex/0503039},
Key = {fds43833}
}
@article{fds365358,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C},
Title = {Search for Higgs bosons decaying into new spin-0 or spin-1
particles in four-lepton final states with the ATLAS
detector with 139 fb −1 of pp collision data at
√s = 13 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2022},
Number = {3},
Year = {2022},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2022)041},
Abstract = {Searches are conducted for new spin-0 or spin-1 bosons using
events where a Higgs boson with mass 125 GeV decays into
four leptons (ℓ = e, μ). This decay is presumed to occur
via an intermediate state which contains two on-shell,
promptly decaying bosons: H → XX/ZX → 4ℓ, where the
new boson X has a mass between 1 and 60 GeV. The search uses
pp collision data collected with the ATLAS detector at the
LHC with an integrated luminosity of 139 fb−1 at a
centre-of-mass energy s = 13 TeV. The data are found to be
consistent with Standard Model expectations. Limits are set
on fiducial cross sections and on the branching ratio of the
Higgs boson to decay into XX/ZX, improving those from
previous publications by a factor between two and four.
Limits are also set on mixing parameters relevant in
extensions of the Standard Model containing a dark sector
where X is interpreted to be a dark boson. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP03(2022)041},
Key = {fds365358}
}
@article{fds321224,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and T. H.
Arce and A and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for higgs bosons decaying to aa in the µµττ final
state in pp collisions at √s = 8 TeV with the ATLAS
experiment},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {5},
Pages = {052002-1-052002-24},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.92.052002},
Abstract = {A search for the decay to a pair of new particles of either
the 125 GeV Higgs boson (h) or a second charge parity
(CP)-even Higgs boson (H) is presented. The data set
corresponds to an integrated luminosity of 20.3 fb-1 of pp
collisions at √s = 8 TeV recorded by the ATLAS experiment
at the LHC in 2012. The search was done in the context of
the next-to-minimal supersymmetric standard model, in which
the new particles are the lightest neutral pseudoscalar
Higgs bosons (a). One of the two a bosons is required to
decay to two muons while the other is required to decay to
two τ leptons. No significant excess is observed above the
expected backgrounds in the dimuon invariant mass range from
3.7 to 50 GeV. Upper limits are placed on the production of
h → aa relative to the standard model gg → h production,
assuming no coupling of the a boson to quarks. The most
stringent limit is placed at 3.5% for ma = 3.75 GeV. Upper
limits are also placed on the production cross section of H
→ aa from 2.33 to 0.72 pb, for fixed ma = 5 GeV with mH
ranging from 100 to 500 GeV.},
Doi = {10.1103/PhysRevD.92.052002},
Key = {fds321224}
}
@article{fds308670,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro,
P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Garcia Sciverez and M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and di
Giovanni, GP and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
C and Giokaris, N and Giolo, K and Giordani, M and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher,
C and Grundler, U and Guimaraes da Costa and J and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer,
A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang,
D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel,
M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Kordas, K and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen,
AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca,
G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin,
M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
A and von der Mey, M and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr,
B and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa,
T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and van Remortel, N and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori, L and Robertson,
WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle,
T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria,
F},
Title = {Search for Higgs bosons decaying to bb and produced in
association with W bosons in pp collisions at square root of
s = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {96},
Number = {8},
Pages = {081803},
Year = {2006},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.96.081803},
Abstract = {We present a search for Higgs bosons decaying into bb and
produced in association with W bosons in pp collisions at
square root of s = 1.96 TeV. This search uses 320 pb(-1) of
the data set accumulated by the upgraded Collider Detector
at Fermilab. Events are selected that have a high-transverse
momentum electron or muon, missing transverse energy, and
two jets, at least one of which is consistent with the
hadronization of a b quark. Both the number of events and
the dijet mass distribution are consistent with standard
model background expectations, and we set 95% confidence
level upper limits on the production cross section times
branching ratio for the Higgs boson or any new particle with
similar decay kinematics. These upper limits range from 10
pb for mH = 110 GeV/c2 to 3 pb for mH = 150
GeV/c2.},
Doi = {10.1103/physrevlett.96.081803},
Key = {fds308670}
}
@article{fds167702,
Author = {M.C. Kruse and D. Hidas and A. Abulencia et al. (CDF
collaboration)},
Title = {Search for Higgs Bosons decaying to pairs of
$W$-Bosons},
Journal = {Phys. Rev. Lett. 102, 021802},
Year = {2009},
Abstract = {http://arxiv.org/abs/0809.3930},
Key = {fds167702}
}
@article{fds308513,
Author = {Aaltonen, T and others},
Title = {Search for Higgs Bosons Predicted in Two-Higgs-Doublet
Models via Decays to Tau Lepton Pairs in 1.96 TeV pp̅
Collisions},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {20},
Pages = {201801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.201801},
Abstract = {We present the results of a search for Higgs bosons
predicted in two-Higgs-doublet models, in the case where the
Higgs bosons decay to tau lepton pairs, using 1.8 fb-1
of integrated luminosity of pp̅ collisions recorded by the
CDF II experiment at the Fermilab Tevatron. Studying the
mass distribution in events where one or both tau leptons
decay leptonically, no evidence for a Higgs boson signal is
observed. The result is used to infer exclusion limits in
the two-dimensional space of tanβ versus mA (the ratio
of the vacuum expectation values of the two Higgs doublets
and the mass of the pseudoscalar boson, respectively).},
Doi = {10.1103/physrevlett.103.201801},
Key = {fds308513}
}
@article{fds308825,
Author = {al, FAE},
Title = {Search for Higgs Bosons Produced in Association with a
Vector Boson in pp collisions at $\sqrt{s} = 1.8
TeV},
Journal = {Physical Review Letters},
Volume = {81},
Number = {26},
Pages = {5748},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.5748},
Abstract = {We search for Higgs bosons produced in association with a
massive vector boson in 91±7pb-1 of pp collisions at √s =
1.8TeV recorded by the Collider Detector at Fermilab. We
assume the Higgs scalar H0 decays to a bb pair with
branching ratio β, and we consider the hadronic decays of
the vector boson V (W or Z). Observations are consistent
with background expectations. We place 95% confidence level
upper limits on σ(pp → H0V)β as a function of the scalar
mass (MH0) over the range 70 < MH0 < 140GeV/c2. When
combined with an analysis of the case where V is a
leptonically decaying W, these limits vary from 23 pb at MH0
= 70GeV/c2 to 17 pb at MH0 = 140GeV/c2. © 1998 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.81.5748},
Key = {fds308825}
}
@article{fds308412,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D},
Title = {Search for Higgs bosons produced in association with b
quarks},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.85.032005},
Abstract = {We present a search for neutral Higgs bosons decaying into
bb̄, produced in association with b quarks in pp̄
collisions. This process could be observable in
supersymmetric models with high values of tanβ. The event
sample corresponds to 2.6fb -1 of integrated luminosity
collected with the CDF II detector at the Fermilab Tevatron
collider. We search for an enhancement in the mass of the
two leading jets in events with three jets identified as
coming from b quarks using a displaced vertex algorithm. A
data-driven procedure is used to estimate the dijet mass
spectrum of the nonresonant multijet background. The
contributions of backgrounds and a possible Higgs boson
signal are determined by a two-dimensional fit of the data,
using the dijet mass together with an additional variable
which is sensitive to the flavor composition of the three
tagged jets. We set mass-dependent limits on
σ(pp̄→)×B(→bb̄) which are applicable for a narrow
scalar particle produced in association with b quarks. We
also set limits on tanβ in supersymmetric Higgs models
including the effects of the Higgs boson width. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.85.032005},
Key = {fds308412}
}
@article{fds308442,
Author = {Aaltonen, and T, and al, E},
Title = {Search for High Mass Resonances Decaying to Muon Pairs in
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$
$p\overline{p}$ Collisions},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {12},
Pages = {121801},
Publisher = {American Physical Society},
Year = {2011},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.121801},
Abstract = {We present a search for a new narrow, spin-1, high mass
resonance decaying to μ(+)μ⁻+X, using a
matrix-element-based likelihood and a simultaneous
measurement of the resonance mass and production rate. In
data with 4.6 fb⁻¹ of integrated luminosity collected by
the CDF detector in pp collisions at √s=1960 GeV, the most
likely signal cross section is consistent with zero at 16%
confidence level. We therefore do not observe evidence for a
high mass resonance and place limits on models predicting
spin-1 resonances, including M>1071 GeV/c² at 95%
confidence level for a Z' boson with the same couplings to
fermions as the Z boson.},
Doi = {10.1103/PhysRevLett.106.121801},
Key = {fds308442}
}
@article{fds321213,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for high-mass diboson resonances with boson-tagged
jets in proton-proton collisions at √s = 8TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {12},
Pages = {1-39},
Publisher = {Springer Nature},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2015)055},
Abstract = {Abstract: A search is performed for narrow resonances
decaying into WW, WZ, or ZZ boson pairs using 20.3 fb−1 of
proton-proton collision data at a centre-of-mass energy of
s=8$$ \sqrt{s}=8 $$ TeV recorded with the ATLAS detector at
the Large Hadron Collider. Diboson resonances with masses in
the range from 1.3 to 3.0 TeV are sought after using the
invariant mass distribution of dijets where both jets are
tagged as a boson jet, compatible with a highly boosted W or
Z boson decaying to quarks, using jet mass and substructure
properties. The largest deviation from a smoothly falling
background in the observed dijet invariant mass distribution
occurs around 2 TeV in the WZ channel, with a global
significance of 2.5 standard deviations. Exclusion limits at
the 95% confidence level are set on the production cross
section times branching ratio for the WZ final state of a
new heavy gauge boson, W′, and for the WW and ZZ final
states of Kaluza-Klein excitations of the graviton in a bulk
Randall-Sundrum model, as a function of the resonance mass.
W′ bosons with couplings predicted by the extended gauge
model in the mass range from 1.3 to 1.5 TeV are excluded at
95% confidence level.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP12(2015)055},
Key = {fds321213}
}
@article{fds314173,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allen, K and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Search for high-mass dilepton resonances in pp collisions at
s =8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {5},
Year = {2014},
Month = {September},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.90.052005},
Abstract = {The ATLAS detector at the Large Hadron Collider is used to
search for high-mass resonances decaying to dielectron or
dimuon final states. Results are presented from an analysis
of proton-proton (pp) collisions at a center-of-mass energy
of 8 TeV corresponding to an integrated luminosity of 20.3
fb-1 in the dimuon channel. A narrow resonance with Standard
Model Z couplings to fermions is excluded at 95% confidence
level for masses less than 2.79 TeV in the dielectron
channel, 2.53 TeV in the dimuon channel, and 2.90 TeV in the
two channels combined. Limits on other model interpretations
are also presented, including a grand-unification model
based on the E6 gauge group, Z∗ bosons, minimal Z′
models, a spin-2 graviton excitation from Randall-Sundrum
models, quantum black holes, and a minimal walking
technicolor model with a composite Higgs
boson.},
Doi = {10.1103/PhysRevD.90.052005},
Key = {fds314173}
}
@article{fds321233,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for high-mass diphoton resonances in pp collisions at
s =8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.92.032004},
Abstract = {This article describes a search for high-mass resonances
decaying to a pair of photons using a sample of 20.3 fb-1 of
pp collisions at s=8 TeV recorded with the ATLAS detector at
the Large Hadron Collider. The data are found to be in
agreement with the Standard Model prediction, and limits are
reported in the framework of the Randall-Sundrum model. This
theory leads to the prediction of graviton states, the
lightest of which could be observed at the Large Hadron
Collider. A lower limit of 2.66 (1.41) TeV at 95% confidence
level is set on the mass of the lightest graviton for
couplings of k/M¯Pl=0.1 (0.01).},
Doi = {10.1103/PhysRevD.92.032004},
Key = {fds321233}
}
@article{fds308535,
Author = {Aaltonen, T and others},
Title = {Search for High-Mass e+e- Resonances in ppbar Collisions at
1.96 TeV},
Journal = {PRL},
Volume = {102},
Number = {3},
Pages = {031801},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.031801},
Abstract = {A search for high-mass resonances in the e+e- final state is
presented based on 2.5 fb(-1) of sqrt[s]=1.96 TeV pp
collision data from the CDF II detector at the Fermilab
Tevatron. The largest excess over the standard model
prediction is at an e+e- invariant mass of 240 GeV/c2. The
probability of observing such an excess arising from
fluctuations in the standard model anywhere in the mass
range of 150-1000 GeV/c2 is 0.6% (equivalent to 2.5sigma).
We exclude the standard model coupling Z' and the
Randall-Sundrum graviton for k/MPl=0.1 with masses below 963
and 848 GeV/c2 at the 95% credibility level,
respectively.},
Doi = {10.1103/physrevlett.102.031801},
Key = {fds308535}
}
@article{fds321153,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for high-mass new phenomena in the dilepton final
state using proton–proton collisions at s=13TeV with the
ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {761},
Pages = {372-392},
Publisher = {Elsevier BV},
Year = {2016},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2016.08.055},
Abstract = {A search is conducted for both resonant and non-resonant
high-mass new phenomena in dielectron and dimuon final
states. The search uses 3.2fb−1 of proton–proton
collision data, collected at s=13TeV by the ATLAS experiment
at the LHC in 2015. The dilepton invariant mass is used as
the discriminating variable. No significant deviation from
the Standard Model prediction is observed; therefore limits
are set on the signal model parameters of interest at 95%
credibility level. Upper limits are set on the cross-section
times branching ratio for resonances decaying to dileptons,
and the limits are converted into lower limits on the
resonance mass, ranging between 2.74 TeV and 3.36 TeV,
depending on the model. Lower limits on the ℓℓqq contact
interaction scale are set between 16.7 TeV and 25.2 TeV,
also depending on the model.},
Doi = {10.1016/j.physletb.2016.08.055},
Key = {fds321153}
}
@article{fds314166,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'Errico, M},
Title = {Search for high-mass resonances decaying into ZZ in pp̄
collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012008},
Abstract = {We search for high-mass resonances decaying into Z boson
pairs using data corresponding to 6fb -1 collected by the
CDF experiment in pp̄ collisions at √s=1.96TeV. The
search is performed in three distinct final states: ZZ→
+-+-, ZZ→ +-νν, and ZZ→ +-jj. For a Randall-Sundrum
graviton G *, the 95% CL upper limits on the production
cross section times branching ratio to ZZ, σ(pp̄→G
*→ZZ), vary between 0.26 pb and 0.045 pb in the mass range
300<M G*<1000GeV/c2. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.85.012008},
Key = {fds314166}
}
@article{fds308532,
Author = {Aaltonen, T and others},
Title = {Search for High-Mass Resonances Decaying to Dimuons at
CDF},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {9},
Pages = {091805},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.091805},
Abstract = {We present a search for high-mass neutral resonances using
dimuon data corresponding to an integrated luminosity of 2.3
fb(-1) collected in pp[over ] collisions at sqrt[s]=1.96 TeV
by the CDF II detector at the Fermilab Tevatron. No
significant excess above the standard model expectation is
observed in the dimuon invariant-mass spectrum. We set 95%
confidence level upper limits on sigmaBR(pp-->X-->micromicro),
where X is a boson with spin-0, 1, or 2. Using these cross
section limits, we determine lower mass limits on sneutrinos
in R-parity-violating supersymmetric models, Z' bosons, and
Kaluza-Klein gravitons in the Randall-Sundrum
model.},
Doi = {10.1103/physrevlett.102.091805},
Key = {fds308532}
}
@article{fds308662,
Author = {Abulencia, and A, and others},
Title = {Search for high-mass resonances decaying to e mu in
$p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {21},
Pages = {211802},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.211802},
Abstract = {We describe a general search for resonances decaying to a
neutral e mu final state in p anti-p collisions at a
center-of-mass energy of 1.96 TeV. Using a data sample
representing 344 pb-1 of integrated luminosity recorded by
the CDF II experiment, we compare Standard Model predictions
with the number of observed events for invariant masses
between 50 and 800 GeV/c2. Finding no significant excess (5
events observed vs. 7.7 +/- 0.8 expected for M_e mu > 100
GeV/c2), we set limits on sneutrino and Z' masses as
functions of lepton family number violating
couplings.},
Doi = {10.1103/physrevlett.96.211802},
Key = {fds308662}
}
@article{fds321276,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H},
Title = {Search for H→γγ produced in association with top quarks
and constraints on the Yukawa coupling between the top quark
and the Higgs boson using data taken at 7 TeV and 8 TeV with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {740},
Pages = {222-242},
Publisher = {Elsevier BV},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2014.11.049},
Abstract = {A search is performed for Higgs bosons produced in
association with top quarks using the diphoton decay mode of
the Higgs boson. Selection requirements are optimized
separately for leptonic and fully hadronic final states from
the top quark decays. The dataset used corresponds to an
integrated luminosity of 4.5 fb−1 of proton–proton
collisions at a center-of-mass energy of 7 TeV and 20.3
fb−1 at 8 TeV recorded by the ATLAS detector at the CERN
Large Hadron Collider. No significant excess over the
background prediction is observed and upper limits are set
on the tt¯H production cross section. The observed
exclusion upper limit at 95% confidence level is 6.7 times
the predicted Standard Model cross section value. In
addition, limits are set on the strength of the Yukawa
coupling between the top quark and the Higgs boson, taking
into account the dependence of the tt¯H and tH cross
sections as well as the H→γγ branching fraction on the
Yukawa coupling. Lower and upper limits at 95% confidence
level are set at −1.3 and +8.0 times the Yukawa coupling
strength in the Standard Model.},
Doi = {10.1016/j.physletb.2014.11.049},
Key = {fds321276}
}
@article{fds314171,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
M},
Title = {Search for invisible decays of a Higgs boson produced in
association with a Z boson in ATLAS},
Journal = {Physical Review Letters},
Volume = {112},
Number = {20},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {May},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.112.201802},
Abstract = {A search for evidence of invisible-particle decay modes of a
Higgs boson produced in association with a Z boson at the
Large Hadron Collider is presented. No deviation from the
standard model expectation is observed in 4.5 fb-1 (20.3
fb-1) of 7 (8) TeV pp collision data collected by the ATLAS
experiment. Assuming the standard model rate for ZH
production, an upper limit of 75%, at the 95% confidence
level is set on the branching ratio to invisible-particle
decay modes of the Higgs boson at a mass of 125.5 GeV. The
limit on the branching ratio is also interpreted in terms of
an upper limit on the allowed dark matter-nucleon scattering
cross section within a Higgs-portal dark matter scenario.
Within the constraints of such a scenario, the results
presented in this Letter provide the strongest available
limits for low-mass dark matter candidates. Limits are also
set on an additional neutral Higgs boson, in the mass range
110 <mH <400 GeV, produced in association with a Z boson and
decaying to invisible particles.},
Doi = {10.1103/PhysRevLett.112.201802},
Key = {fds314171}
}
@article{fds321301,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
Title = {Search for invisible decays of the Higgs boson produced in
association with a hadronically decaying vector boson in
pp collisions at [Formula: see text] TeV with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {337},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3551-1},
Abstract = {A search for Higgs boson decays to invisible particles is
performed using 20.3 [Formula: see text] of <i>pp</i>
collision data at a centre-of-mass energy of 8 TeV recorded
by the ATLAS detector at the Large Hadron Collider. The
process considered is Higgs boson production in association
with a vector boson ([Formula: see text] or <i>Z</i>) that
decays hadronically, resulting in events with two or more
jets and large missing transverse momentum. No excess of
candidates is observed in the data over the background
expectation. The results are used to constrain <i>VH</i>
production followed by <i>H</i> decaying to invisible
particles for the Higgs boson mass range [Formula: see
text] GeV. The 95 % confidence-level observed upper limit
on [Formula: see text] varies from 1.6 pb at 115 GeV to
0.13 pb at 300 GeV. Assuming Standard Model production and
including the [Formula: see text] contribution as signal,
the results also lead to an observed upper limit of 78 % at
95 % confidence level on the branching ratio of Higgs
bosons decays to invisible particles at a mass of
125 GeV.},
Doi = {10.1140/epjc/s10052-015-3551-1},
Key = {fds321301}
}
@article{fds321287,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos,
G and Azuma, Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek,
P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil,
HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell,
WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S},
Title = {Search for invisible particles produced in association with
single-top-quarks in proton-proton collisions at [Formula:
see text] with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {2},
Pages = {79},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3233-4},
Abstract = {A search for the production of single-top-quarks in
association with missing energy is performed in
proton-proton collisions at a centre-of-mass energy of
[Formula: see text] with the ATLAS experiment at the large
hadron collider using data collected in 2012, corresponding
to an integrated luminosity of [Formula: see
text] fb[Formula: see text]. In this search, the [Formula:
see text] boson from the top quark is required to decay into
an electron or a muon and a neutrino. No deviation from the
standard model prediction is observed, and upper limits are
set on the production cross-section for resonant and
non-resonant production of an invisible exotic state in
association with a right-handed top quark. In the case of
resonant production, for a spin-[Formula: see text]
resonance with a mass of [Formula: see text] GeV, an
effective coupling strength above [Formula: see text] is
excluded at 95[Formula: see text] confidence level for the
top quark and an invisible spin-[Formula: see text] state
with mass between [Formula: see text] and [Formula: see
text] GeV. In the case of non-resonant production, an
effective coupling strength above [Formula: see text] is
excluded at 95[Formula: see text] confidence level for the
top quark and an invisible spin-[Formula: see text] state
with mass between [Formula: see text] and [Formula: see
text] GeV.},
Doi = {10.1140/epjc/s10052-014-3233-4},
Key = {fds321287}
}
@article{fds308733,
Author = {Collaboration, DAEACDFII},
Title = {Search for Kaluza-Klein Graviton Emission in pp-bar
Collisions at sqrt[s]=1.8 TeV Using the Missing Energy
Signature},
Journal = {Physical Review Letters},
Volume = {92},
Number = {12},
Pages = {121802},
Year = {2004},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.92.121802},
Abstract = {We report on a search for direct Kaluza-Klein graviton
production in a data sample of 84 pb-1 of pp-bar collisions
at sqrt[s]=1.8 TeV, recorded by the Collider Detector at
Fermilab. We investigate the final state of large missing
transverse energy and one or two high energy jets. We
compare the data with the predictions from a
(3+1+n)-dimensional Kaluza-Klein scenario in which gravity
becomes strong at the TeV scale. At 95% confidence level
(C.L.) for n=2, 4, and 6 we exclude an effective Planck
scale below 1.0, 0.77, and 0.71 TeV, respectively.},
Doi = {10.1103/physrevlett.92.121802},
Key = {fds308733}
}
@article{fds308656,
Author = {Abulencia, and A, and others},
Title = {Search for large extra dimensions in the production of jets
and missing transverse energy in $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {97},
Number = {17},
Pages = {171802},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.97.171802},
Abstract = {We present the results of a search for new physics in the
jets plus missing transverse energy data sample collected
from 368 pb-1 of p anti-p collisions at s**(1/2) = 1.96 TeV
recorded by the Collider Detector at Fermilab. We compare
the number of events observed in the data with a data-based
estimate of the standard model backgrounds contributing to
this signature. We observe no significant excess of events,
and we interpret this null result in terms of lower limits
on the fundamental Planck scale for a large extra dimensions
scenario.},
Doi = {10.1103/physrevlett.97.171802},
Key = {fds308656}
}
@article{fds308753,
Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Bensinger, J and Beretvas, A and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Bromberg, C and Brozovic, M and Brubaker,
E and Bruner, N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers,
W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R and Dagenhart, D and D'Auria, S and Cecco, SD and Jongh, FD and dell'Agnello, S and dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo,
T and Eddy, N and Einsweiler, K and Jr, EE and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fan, Q and Farrington, S and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher,
B and Flores-Castillo, LR and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Gerstein, E and Giagu, S and Giannetti, P and Giolo, K and Giordani, M and Giromini, P and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Gresele, A and Grim, G and Grosso-Pilcher,
C and Guenther, M and Guillian, G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Halkiadakis, E and Hall, C and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Hennecke,
M and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hollebeek,
R and Holloway, L and Hou, S and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Issever, C and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iwai, J and Iwata, Y and Iyutin, B and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Kang,
J and Unel, MK and Karr, K and Kartal, S and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, TH and Kim, YK and Kirby,
M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kotelnikov, K and Kovacs,
E and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kurino,
K and Kuwabara, T and Kuznetsova, N and Laasanen, AT and Lai, N and Lami,
S and Lammel, S and Lancaster, J and Lannon, K and Lancaster, M and Lander,
R and Lath, A and Latino, G and LeCompte, T and Le, Y and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, CS and Lindgren,
M and Liss, TM and Liu, JB and Liu, T and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, NS and Loginov, A and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak,
R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Manca, G and Mariotti, M and Martignon, G and Martin, M and Martin, A and Martin, V and Martínez, M and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Miyazaki, Y and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Napora, R and Niell, F and Nelson,
C and Nelson, T and Neu, C and Neubauer, MS and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nigmanov, T and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Pescara, L and Phillips, TJ and Piacentino,
G and Piedra, J and Pitts, KT and Pompoš, A and Pondrom, L and Pope, G and Pratt, T and Prokoshin, F and Proudfoot, J and Ptohos, F and Pukhov, O and Punzi, G and Rademacker, J and Rakitine, A and Ratnikov, F and Ray, H and Reher, D and Reichold, A and Renton, P and Rescigno, M and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson,
WJ and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Ryan, D and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi,
L and Sarkar, S and Sato, H and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
AJ and Sliwa, K and Snider, FD and Snihur, R and Solodsky, A and Speer, T and Spezziga, M and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sukhanov, A and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, RJ and Teng, PK and Terashi,
K and Tether, S and Thom, J and Thompson, AS and Thomson, E and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tonelli, D and Tonnesmann, M and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Tsybychev, D and Turini,
N and Ukegawa, F and Unverhau, T and Vaiciulis, T and Valls, J and Varganov, A and Vataga, E and Vejcik, S and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D},
Title = {Search for Lepton Flavor Violating Decays of a Heavy Neutral
Particle in p p̄ Collisions at √s = 1.8
TeV},
Journal = {Physical Review Letters},
Volume = {91},
Number = {17},
Pages = {1716021-1716026},
Year = {2003},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.91.171602},
Abstract = {Lepton flavor violating decays of a heavy neutral particle
in pp̄ collisions at √s = 1.8 TeV were studied. The
position of PP̄ collisions along the beam line was measured
in the vertex time projection chamber (VTX). The results
show no evidence for new particles with lepton flavor
violating decays. The limits on the cross section for
production and decay of single sneutrino with R-parity
violating interactions were also set.},
Doi = {10.1103/physrevlett.91.171602},
Key = {fds308753}
}
@article{fds308749,
Author = {Collaboration, DAEACDF},
Title = {Search for Long-Lived Charged Massive Particles in pp-bar
Collisions at sqrt[s]=1.8 TeV},
Journal = {Physical Review Letters},
Volume = {90},
Number = {13},
Pages = {131801},
Year = {2003},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.90.131801},
Abstract = {We report a search for the production of long-lived charged
massive particles in a data sample of 90 pb-1 of sqrt[s]=1.8
TeV pp-bar collisions recorded by the Collider Detector at
Fermilab. The search uses the muonlike penetration and
anomalously high ionization energy loss signature expected
for such a particle to discriminate it from backgrounds. The
data are found to agree with background expectations, and
cross section limits of O(1) pb are derived using two
reference models, a stable quark and a stable scalar
lepton.},
Doi = {10.1103/physrevlett.90.131801},
Key = {fds308749}
}
@article{fds365352,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling, JH},
Title = {Search for long-lived charginos based on a
disappearing-track signature using 136 fb - 1 of
pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {7},
Year = {2022},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10489-5},
Abstract = {A search for long-lived charginos produced either directly
or in the cascade decay of heavy prompt gluino states is
presented. The search is based on proton–proton collision
data collected at a centre-of-mass energy of s = 13 TeV
between 2015 and 2018 with the ATLAS detector at the LHC,
corresponding to an integrated luminosity of 136 fb- 1.
Long-lived charginos are characterised by a distinct
signature of a short and then disappearing track, and are
reconstructed using at least four measurements in the ATLAS
pixel detector, with no subsequent measurements in the
silicon-microstrip tracking volume nor any associated energy
deposits in the calorimeter. The final state is complemented
by a large missing transverse-momentum requirement for
triggering purposes and at least one high-transverse-momentum
jet. No excess above the expected backgrounds is observed.
Exclusion limits are set at 95% confidence level on the
masses of the chargino and gluino for different chargino
lifetimes. Chargino masses up to 660 (210) GeV are
excluded in scenarios where the chargino is a pure wino
(higgsino). For charginos produced during the cascade decay
of a heavy gluino, gluinos with masses below 2.1 TeV are
excluded for a chargino mass of 300 GeV and a lifetime of
0.2 ns.},
Doi = {10.1140/epjc/s10052-022-10489-5},
Key = {fds365352}
}
@article{fds308523,
Author = {Aaltonen, T and others},
Title = {Search for Long-Lived Massive Charged Particles in 1.96 TeV
pp̅ Collisions},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {2},
Pages = {021802},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.021802},
Abstract = {We performed a signature-based search for long-lived charged
massive particles produced in 1.0 fb-1 of pp̅
collisions at sqrt[s]=1.96 TeV, collected with the CDF
II detector using a high transverse-momentum (pT) muon
trigger. The search used time of flight to isolate slowly
moving, high-pT particles. One event passed our selection
cuts with an expected background of 1.9 ± 0.2 events.
We set an upper bound on the production cross section and,
interpreting this result within the context of a stable
scalar top-quark model, set a lower limit on the particle
mass of 249 GeV/c2 at 95% C.L.},
Doi = {10.1103/physrevlett.103.021802},
Key = {fds308523}
}
@article{fds321319,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for long-lived neutral particles decaying into lepton
jets in proton-proton collisions at √s= 8TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {11},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP11(2014)088},
Abstract = {Abstract: Several models of physics beyond the Standard
Model predict neutral particles that decay into final states
consisting of collimated jets of light leptons and hadrons
(so-called “lepton jets”). These particles can also be
long-lived with decay length comparable to, or even larger
than, the LHC detectors’ linear dimensions. This paper
presents the results of a search for lepton jets in
proton-proton collisions at the centre-of-mass energy of
√s= 8TeV in a sample of 20.3 fb−1 collected during 2012
with the ATLAS detector at the LHC. Limits on models
predicting Higgs boson decays to neutral long-lived lepton
jets are derived as a function of the particle’s proper
decay length.},
Doi = {10.1007/JHEP11(2014)088},
Key = {fds321319}
}
@article{fds308837,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and De Barbara and P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Culbertson, R and Dagenhart, D and Daniels, T and Dejongh, F and Dell'Agnello, S and Dell'Orso, M},
Title = {Search for long-lived parents of Z° bosons inpp collisions
at √s = 1.8 TeV},
Journal = {Physical Review D},
Volume = {58},
Number = {5},
Pages = {511021-511025},
Year = {1998},
Month = {January},
ISSN = {0556-2821},
Abstract = {We search for new long-lived particles which decay to Z0
bosons by looking for Z0→e+e- decays with displaced
vertices. We find no evidence for parent particles pf the Z0
with long lifetimes in 90 pb-1 of data from the CDF
experiment at Fermilab. We set a cross section limit as a
function of the lifetime of the parent particle for both a
generic Z0 parent and a fourth-generation, charge -1/3 quark
that decays into Z0b. © 1998 The American Physical
Society.},
Key = {fds308837}
}
@article{fds308293,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Search for long-lived stopped R-hadrons decaying out of time
with pp collisions using the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {11},
Pages = {112003-1-112003-30},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.88.112003},
Abstract = {An updated search is performed for gluino, top squark, or
bottom squark R-hadrons that have come to rest within the
ATLAS calorimeter, and decay at some later time to hadronic
jets and a neutralino, using 5.0 and 22:9 fb-1 of pp
collisions at 7 and 8 TeV, respectively. Candidate decay
events are triggered in selected empty bunch crossings of
the LHC in order to remove pp collision backgrounds.
Selections based on jet shape and muon system activity are
applied to discriminate signal events from cosmic ray and
beam-halo muon backgrounds. In the absence of an excess of
events, improved limits are set on gluino, stop, and sbottom
masses for different decays, lifetimes, and neutralino
masses. With a neutralino of mass 100 GeV, the analysis
excludes gluinos with mass below 832 GeV (with an expected
lower limit of 731 GeV), for a gluino lifetime between 10
μs and 1000 s in the generic R-hadron model with equal
branching ratios for decays to (formula presented) and
(formula presented). Under the same assumptions for the
neutralino mass and squark lifetime, top squarks and bottom
squarks in the Regge R-hadron model are excluded with masses
below 379 and 344 GeV, respectively.},
Doi = {10.1103/PhysRevD.88.112003},
Key = {fds308293}
}
@article{fds308346,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
ATH and Arfaoui, S and Arguin, JF and Arik, E},
Title = {Search for long-lived, heavy particles in final states with
a muon and multi-track displaced vertex in proton-proton
collisions at √s=7 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {719},
Number = {4-5},
Pages = {280-298},
Publisher = {Elsevier BV},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.042},
Abstract = {Many extensions of the Standard Model posit the existence of
heavy particles with long lifetimes. In this Letter, results
are presented of a search for events containing one or more
such particles, which decay at a significant distance from
their production point, using a final state containing
charged hadrons and an associated muon. This analysis uses a
data sample of proton-proton collisions at s=7TeV
corresponding to an integrated luminosity of 4.4 fb−1
collected in 2011 by the ATLAS detector operating at the
Large Hadron Collider. Results are interpreted in the
context of R-parity violating supersymmetric scenarios. No
events in the signal region are observed and limits are set
on the production cross section for pair production of
supersymmetric particles, multiplied by the square of the
branching fraction for a neutralino to decay to charged
hadrons and a muon, based on the scenario where both of the
produced supersymmetric particles give rise to neutralinos
that decay in this way. However, since the search strategy
is based on triggering on and reconstructing the decay
products of individual long-lived particles, irrespective of
the rest of the event, these limits can easily be
reinterpreted in scenarios with different numbers of
long-lived particles per event. The limits are presented as
a function of neutralino lifetime, and for a range of squark
and neutralino masses.},
Doi = {10.1016/j.physletb.2013.01.042},
Key = {fds308346}
}
@article{fds321241,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for long-lived, weakly interacting particles that
decay to displaced hadronic jets in proton-proton collisions
at s =8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.92.012010},
Abstract = {A search for the decay of neutral, weakly interacting,
long-lived particles using data collected by the ATLAS
detector at the LHC is presented. This analysis uses the
full data set recorded in 2012: 20.3 fb-1 of proton-proton
collision data at s=8 TeV. The search employs techniques for
reconstructing decay vertices of long-lived particles
decaying to jets in the inner tracking detector and muon
spectrometer. Signal events require at least two
reconstructed vertices. No significant excess of events over
the expected background is found, and limits as a function
of proper lifetime are reported for the decay of the Higgs
boson and other scalar bosons to long-lived particles and
for Hidden Valley Z′ and Stealth SUSY benchmark models.
The first search results for displaced decays in Z′ and
Stealth SUSY models are presented. The upper bounds of the
excluded proper lifetimes are the most stringent to
date.},
Doi = {10.1103/PhysRevD.92.012010},
Key = {fds321241}
}
@article{fds321243,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for low-scale gravity signatures in multi-jet final
states with the ATLAS detector at √s =
8TeV},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {7},
Publisher = {Springer Nature},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2015)032},
Abstract = {A search for evidence of physics beyond the Standard Model
in final states with multiple high-transverse-momentum jets
is performed using 20.3 fb−1 of proton-proton collision
data at (Formula presented.) = 8 TeV recorded by the ATLAS
detector at the LHC. No significant excess of events beyond
Standard Model expectations is observed, and upper limits on
the visible cross sections for non-Standard Model production
of multi-jet final states are set. A wide variety of models
for black hole and string ball production and decay are
considered, and the upper limit on the cross section times
acceptance is as low as 0.16 fb at the 95% confidence level.
For these models, excluded regions are also given as
function of the main model parameters.},
Doi = {10.1007/JHEP07(2015)032},
Key = {fds321243}
}
@article{fds315438,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for magnetic monopoles and stable particles with high
electric charges in 8 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {93},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {March},
ISSN = {2470-0010},
url = {http://dx.doi.org/10.1103/PhysRevD.93.052009},
Abstract = {A search for highly ionizing particles produced in
proton-proton collisions at 8 TeV center-of-mass energy is
performed by the ATLAS Collaboration at the CERN Large
Hadron Collider. The data set used corresponds to an
integrated luminosity of 7.0 fb-1. A customized trigger
significantly increases the sensitivity, permitting a search
for such particles with charges and energies beyond what was
previously accessible. No events were found in the signal
region, leading to production cross section upper limits in
the mass range 200-2500 GeV for magnetic monopoles with
magnetic charge in the range 0.5gD<|g|<2.0gD, where gD is
the Dirac charge, and for stable particles with electric
charge in the range 10<|z|<60. Model-dependent limits are
presented in given pair-production scenarios, and
model-independent limits are presented in fiducial regions
of particle energy and pseudorapidity.},
Doi = {10.1103/PhysRevD.93.052009},
Key = {fds315438}
}
@article{fds375907,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury,
KA and Alberghi, GL and Albert, J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Search for Majorana neutrinos in same-sign WW scattering
events from pp collisions at √s=13 TeV},
Journal = {European Physical Journal C},
Volume = {83},
Number = {9},
Year = {2023},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11915-y},
Abstract = {A search for Majorana neutrinos in same-sign WW scattering
events is presented. The analysis uses s=13 TeV
proton–proton collision data with an integrated luminosity
of 140 fb - 1 recorded during 2015–2018 by the ATLAS
detector at the Large Hadron Collider. The analysis targets
final states including exactly two same-sign muons and at
least two hadronic jets well separated in rapidity. The
modelling of the main backgrounds, from Standard Model
same-sign WW scattering and WZ production, is constrained
with data in dedicated signal-depleted control regions. The
distribution of the transverse momentum of the
second-hardest muon is used to search for signals
originating from a heavy Majorana neutrino with a mass
between 50 GeV and 20 TeV. No significant excess is
observed over the background expectation. The results are
interpreted in a benchmark scenario of the Phenomenological
Type-I Seesaw model. In addition, the sensitivity to the
Weinberg operator is investigated. Upper limits at the 95%
confidence level are placed on the squared
muon-neutrino–heavy-neutrino mass-mixing matrix element |
VμN| 2 as a function of the heavy Majorana neutrino’s
mass mN , and on the effective μμ Majorana neutrino mass |
mμμ| .},
Doi = {10.1140/epjc/s10052-023-11915-y},
Key = {fds375907}
}
@article{fds321250,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for massive supersymmetric particles decaying to many
jets using the ATLAS detector in pp collisions at s =8
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.91.112016},
Abstract = {Results of a search for decays of massive particles to fully
hadronic final states are presented. This search uses 20.3
fb-1 of data collected by the ATLAS detector in s=8 TeV
proton-proton collisions at the LHC. Signatures based on
high jet multiplicities without requirements on the missing
transverse momentum are used to search for
R-parity-violating supersymmetric gluino pair production
with subsequent decays to quarks. The analysis is performed
using a requirement on the number of jets, in combination
with separate requirements on the number of b-tagged jets,
as well as a topological observable formed from the scalar
sum of the mass values of large-radius jets in the event.
Results are interpreted in the context of all possible
branching ratios of direct gluino decays to various quark
flavors. No significant deviation is observed from the
expected Standard Model backgrounds estimated using jet
counting as well as data-driven templates of the
total-jet-mass spectra. Gluino pair decays to ten or more
quarks via intermediate neutralinos are excluded for a
gluino with mass mg<1 TeV for a neutralino mass mχ10=500
GeV. Direct gluino decays to six quarks are excluded for
mg<917 GeV for light-flavor final states, and results for
various flavor hypotheses are presented.},
Doi = {10.1103/PhysRevD.91.112016},
Key = {fds321250}
}
@article{fds314189,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for massive, long-lived particles using multitrack
displaced vertices or displaced lepton pairs in pp
collisions at s =8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {October},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.92.072004},
Abstract = {Many extensions of the Standard Model posit the existence of
heavy particles with long lifetimes. This article presents
the results of a search for events containing at least one
long-lived particle that decays at a significant distance
from its production point into two leptons or into five or
more charged particles. This analysis uses a data sample of
proton-proton collisions at s=8 TeV corresponding to an
integrated luminosity of 20.3 fb-1 collected in 2012 by the
ATLAS detector operating at the Large Hadron Collider. No
events are observed in any of the signal regions, and limits
are set on model parameters within supersymmetric scenarios
involving R-parity violation, split supersymmetry, and gauge
mediation. In some of the search channels, the trigger and
search strategy are based only on the decay products of
individual long-lived particles, irrespective of the rest of
the event. In these cases, the provided limits can easily be
reinterpreted in different scenarios.},
Doi = {10.1103/PhysRevD.92.072004},
Key = {fds314189}
}
@article{fds308533,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bar-Shalom, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar, P and Behari, S and Bellettini, G and Bellinger,
J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry,
T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'orso,
M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent,
PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia,
JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare,
M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun,
SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato,
Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson,
B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus, J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone,
S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen,
D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli,
F and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Movilla
Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rajaraman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard,
PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
I and Sidoti, A and Sinervo, P and Sisakyan, A},
Title = {Search for maximal flavor violating scalars in same-charge
lepton pairs in pp collisions at sqrt[s]=1.96
TeV.},
Journal = {Physical review letters},
Volume = {102},
Number = {4},
Pages = {041801},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.102.041801},
Abstract = {Models of maximal flavor violation (MxFV) in elementary
particle physics may contain at least one new scalar SU(2)
doublet field Phi(FV)=(eta(0),eta(+)) that couples the first
and third generation quarks (q_(1), q_(3)) via a Lagrangian
term L(FV)=xi(13)Phi(FV)q(1)q(3). These models have a
distinctive signature of same-charge top-quark pairs and
evade flavor-changing limits from meson mixing measurements.
Data corresponding to 2 fb(-1) collected by the Collider
Dectector at Fermilab II detector in pp[over ] collisions at
sqrt[s]=1.96 TeV are analyzed for evidence of the MxFV
signature. For a neutral scalar eta(0) with m_(eta;(0))=200
GeV/c(2) and coupling xi(13)=1, approximately 11 signal
events are expected over a background of 2.1+/-1.8 events.
Three events are observed in the data, consistent with
background expectations, and limits are set on the coupling
xi(13) for m(eta(0)=180-300 GeV/c(2).},
Doi = {10.1103/physrevlett.102.041801},
Key = {fds308533}
}
@article{fds321306,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
Title = {Search for metastable heavy charged particles with large
ionisation energy loss in pp collisions at [Formula:
see text] TeV using the ATLAS experiment.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {9},
Pages = {407},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3609-0},
Abstract = {Many extensions of the Standard Model predict the existence
of charged heavy long-lived particles, such as
<i>R</i>-hadrons or charginos. These particles, if produced
at the Large Hadron Collider, should be moving
non-relativistically and are therefore identifiable through
the measurement of an anomalously large specific energy loss
in the ATLAS pixel detector. Measuring heavy long-lived
particles through their track parameters in the vicinity of
the interaction vertex provides sensitivity to metastable
particles with lifetimes from 0.6 ns to 30 ns. A search
for such particles with the ATLAS detector at the Large
Hadron Collider is presented, based on a data sample
corresponding to an integrated luminosity of [Formula: see
text] fb[Formula: see text] of <i>pp</i> collisions at
[Formula: see text] TeV. No significant deviation from the
Standard Model background expectation is observed, and
lifetime-dependent upper limits on <i>R</i>-hadrons and
chargino production are set. Gluino <i>R</i>-hadrons with
10 ns lifetime and masses up to 1185 GeV are excluded at
95 [Formula: see text] confidence level, and so are
charginos with 15 ns lifetime and masses up to
482 GeV.},
Doi = {10.1140/epjc/s10052-015-3609-0},
Key = {fds321306}
}
@article{fds321196,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for metastable heavy charged particles with large
ionization energy loss in pp collisions at s =13 TeV using
the ATLAS experiment},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112015},
Abstract = {This paper presents a search for massive charged long-lived
particles produced in pp collisions at s=13 TeV at the LHC
using the ATLAS experiment. The data set used corresponds to
an integrated luminosity of 3.2 fb-1. Many extensions of the
Standard Model predict the existence of massive charged
long-lived particles, such as R-hadrons. These massive
particles are expected to be produced with a velocity
significantly below the speed of light, and therefore to
have a specific ionization higher than any Standard Model
particle of unit charge at high momenta. The Pixel subsystem
of the ATLAS detector is used to measure the ionization
energy loss of reconstructed charged particles and to search
for such highly ionizing particles. The search presented
here has much greater sensitivity than a similar search
performed using the ATLAS detector in the s=8 TeV data set,
thanks to the increase in expected signal cross section due
to the higher center-of-mass energy of collisions, to an
upgraded detector with a new silicon layer close to the
interaction point, and to analysis improvements. No
significant deviation from Standard Model background
expectations is observed, and lifetime-dependent upper
limits on R-hadron production cross sections and masses are
set. Gluino R-hadrons with lifetimes above 0.4 ns and
decaying to qq plus a 100 GeV neutralino are excluded at the
95% confidence level, with lower mass limit ranging between
740 and 1590 GeV. In the case of stable R-hadrons the lower
mass limit at the 95% confidence level is 1570
GeV.},
Doi = {10.1103/PhysRevD.93.112015},
Key = {fds321196}
}
@article{fds321340,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for microscopic black holes and string balls in final
states with leptons and jets with the ATLAS detector at √s
= 8 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {8},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP08(2014)103},
Abstract = {A search for an excess of events with multiple high
transverse momentum objects including charged leptons and
jets is presented, using 20.3 fb -1 of proton-proton
collision data recorded by the ATLAS detector at the Large
Hadron Collider in 2012 at a centre-of-mass energy of √s =
8 TeV. No excess of events beyond Standard Model
expectations is observed. Using extra-dimensional models for
black hole and string ball production and decay, exclusion
contours are determined as a function of the mass threshold
for production and the fundamental gravity scale for two,
four and six extra dimensions. For six extra dimensions,
mass thresholds of 4.8-6.2 TeV are excluded at 95 %
confidence level, depending on the fundamental gravity scale
and model assumptions. Upper limits on the fiducial
cross-sections for non-Standard Model production of these
final states are set. [Figure not available: see fulltext.]
© 2014 The Author(s).},
Doi = {10.1007/JHEP08(2014)103},
Key = {fds321340}
}
@article{fds308307,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Search for microscopic black holes in a like-sign dimuon
final state using large track multiplicity with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.88.072001},
Abstract = {A search is presented for microscopic black holes in a
like-sign dimuon final state in proton-proton collisions at
√s=8 TeV. The data were collected with the ATLAS detector
at the Large Hadron Collider in 2012 and correspond to an
integrated luminosity of 20.3 fb-1. Using a high track
multiplicity requirement, 0.6±0.2 background events from
Standard Model processes are predicted and none observed.
This result is interpreted in the context of low-scale
gravity models and 95% C.L. lower limits on microscopic
black hole masses are set for different model assumptions.
© 2013 CERN. Published by the American Physical Society
under the terms of the Creative Commons Attribution 3.0
License. Further distribution of this work must maintain
attribution to the author(s) and the published article's
title, journal citation, and DOI.},
Doi = {10.1103/PhysRevD.88.072001},
Key = {fds308307}
}
@article{fds321147,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Baarreiro Guimrães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Billoud, TRV and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
Title = {Search for minimal supersymmetric standard model Higgs
Bosons H / A and for a [Formula: see text] boson in the
[Formula: see text] final state produced in pp collisions at
[Formula: see text] TeV with the ATLAS detector.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {11},
Pages = {585},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4400-6},
Abstract = {A search for neutral Higgs bosons of the minimal
supersymmetric standard model (MSSM) and for a heavneutral
[Formula: see text] boson is performed using a data sample
corresponding to an integrated luminosity of
3.2 fb[Formula: see text] from proton-proton collisions at
[Formula: see text] [Formula: see text] recorded by the
ATLAS detector at the LHC. The heavy resonance is assumed to
decay to a [Formula: see text] pair with at least one
[Formula: see text] lepton decaying to final states with
hadrons and a neutrino. The search is performed in the mass
range of 0.2-1.2 [Formula: see text] for the MSSM neutral
Higgs bosons and 0.5-2.5 [Formula: see text] for the
heavy neutral [Formula: see text] boson. The data are in
good agreement with the background predicted by the Standard
Model. The results are interpreted in MSSM and [Formula: see
text] benchmark scenarios. The most stringent constraints on
the MSSM [Formula: see text]-[Formula: see text] space
exclude at 95 % confidence level (CL) [Formula: see text]
for [Formula: see text] [Formula: see text] in the
[Formula: see text] MSSM scenario. For the Sequential
Standard Model, a [Formula: see text] mass up to
1.90 [Formula: see text] is excluded at 95 % CL and
masses up to 1.82-2.17 [Formula: see text] are excluded
for a [Formula: see text] of the strong flavour
model.},
Doi = {10.1140/epjc/s10052-016-4400-6},
Key = {fds321147}
}
@article{fds337971,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbara, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson,
R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin,
T and Dittmann, JR and Dominguez, A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erbacher, R and Errede, D and Errede, S and Fan, Q and Feild,
RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman,
J and Frisch, HJ and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov,
I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian,
G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa,
T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis, JD and Lindgren,
M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos, A and Pondrom,
L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos,
F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Rossin, R and Roy, A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez,
C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott,
A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti, A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Steele, J and Stefanini,
A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki,
T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup,
A and Tonelli, D and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng,
J and Turini, N and Ukegawa, F and Vaiciulis, T and Valls, J and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and III,
WCW and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Search for narrow diphoton resonances and for γγ+W/Z
signatures in pp̄ collisions at √s = 1.8
TeV},
Journal = {Physical Review D},
Volume = {64},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2001},
url = {http://dx.doi.org/10.1103/PhysRevD.64.092002},
Abstract = {We present results of searches for diphoton resonances
produced both inclusively and also in association with a
vector boson (W or Z) using 100 pb-1 of pp̄ collisions
using the CDF detector. We set upper limits on the product
of cross section times branching ratio for both
pp̄→γγ+X and pp̄→γγ+ W/Z. Comparing the inclusive
production to the expectations from heavy sgoldstinos we
derive limits on the supersymmetry-breaking scale √F in
the TeV range, depending on the sgoldstino mass and the
choice of other parameters. Also, using a NLO prediction for
the associated production of a Higgs boson with a W or Z
boson, we set an upper limit on the branching ratio for H
→ γγ. Finally, we set a lower limit on the mass of a
"bosophilic" Higgs boson (e.g., one which couples only to
γ, W, and Z bosons with standard model couplings) of 82
GeV/c2 at 95% confidence level. ©2001 The American Physical
Society.},
Doi = {10.1103/PhysRevD.64.092002},
Key = {fds337971}
}
@article{fds308568,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D},
Title = {Search for narrow resonances lighter than Υ
mesons},
Journal = {European Physical Journal C},
Volume = {62},
Number = {2},
Pages = {319-326},
Publisher = {Springer Nature},
Year = {2009},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-009-1057-4},
Abstract = {We report a search for narrow resonances, produced in p p̄
collisions at √ s=1.96 TeV, that decay into muon pairs
with invariant mass between 6.3 and 9.0 GeV/c 2. The data,
collected with the CDF II detector at the Fermilab Tevatron
collider, correspond to an integrated luminosity of 630 pb
-1. We use the dimuon invariant mass distribution to set 90%
upper credible limits of about 1% to the ratio of the
production cross section times muonic branching fraction of
possible narrow resonances to that of the Υ(1S) meson. ©
2009 Springer-Verlag.},
Doi = {10.1140/epjc/s10052-009-1057-4},
Key = {fds308568}
}
@article{fds308373,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Lvarez
González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler,
M and Buescher, V and Bunichev, V and Burdin, S},
Title = {Search for neutral Higgs bosons in events with multiple
bottom quarks at the Tevatron},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.86.091101},
Abstract = {The combination of searches performed by the CDF and D0
collaborations at the Fermilab Tevatron Collider for neutral
Higgs bosons produced in association with b quarks is
reported. The data, corresponding to 2.6fb -1 of integrated
luminosity at CDF and 5.2fb -1 at D0, have been collected in
final states containing three or more b jets. Upper limits
are set on the cross section multiplied by the branching
ratio varying between 44 pb and 0.7 pb in the Higgs boson
mass range 90 to 300 GeV, assuming production of a narrow
scalar boson. Significant enhancements to the production of
Higgs bosons can be found in theories beyond the standard
model, for example, in supersymmetry. The results are
interpreted as upper limits in the parameter space of the
minimal supersymmetric standard model in a benchmark
scenario favoring this decay mode. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.091101},
Key = {fds308373}
}
@article{fds308674,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and Daronco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann, J and Dituro,
P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Garcia Sciveres and M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
da Costa, J and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer, A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel, M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong,
DJ and Konigsberg, J and Kordas, K and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and Lecompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis,
JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss,
TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, F and Marginean, R and Marino,
C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama,
T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and von der Mey, M and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman,
R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov,
AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and van Remortel, N and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov,
A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi,
I},
Title = {Search for neutral Higgs bosons of the minimal
supersymmetric standard model decaying to tau pairs in pp
collisions at square root of s = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {96},
Number = {1},
Pages = {011802},
Year = {2006},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.96.011802},
Abstract = {We present a search for neutral supersymmetric Higgs bosons
decaying to tau pairs produced in pp collisions at square
root of s = 1.96 TeV. The data, corresponding to 310 pb(-1)
integrated luminosity, were collected with the Collider
Detector at Fermilab in run II of the Tevatron. No
significant excess above the standard model backgrounds is
observed. We set exclusion limits on the production cross
section times branching fraction to tau pairs for Higgs
boson masses in the range from 90 to 250
GeV/c2.},
Doi = {10.1103/physrevlett.96.011802},
Key = {fds308674}
}
@article{fds321318,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Search for neutral Higgs bosons of the minimal
supersymmetric standard model in pp collisions at vs= 8TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {11},
Pages = {1-47},
Publisher = {Springer Nature},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2014)056},
Abstract = {Abstract: A search for the neutral Higgs bosons predicted by
the Minimal Supersymmetric Standard Model (MSSM) is
reported. The analysis is performed on data from
proton-proton collisions at a centre-of-mass energy of 8 TeV
collected with the ATLAS detector at the Large Hadron
Collider. The samples used for this search were collected in
2012 and correspond to integrated luminosities in the range
19.5-20.3 fb−1. The MSSM Higgs bosons are searched for in
the τ τ final state. No significant excess over the
expected background is observed, and exclusion limits are
derived for the production cross section times branching
fraction of a scalar particle as a function of its mass. The
results are also interpreted in the MSSM parameter space for
various benchmark scenarios.},
Doi = {10.1007/JHEP11(2014)056},
Key = {fds321318}
}
@article{fds308427,
Author = {Aaltonen, TEA},
Title = {Search for New ${T}^\prime$ Particles in Final States with
Large Jet Multiplicities and Missing Transverse Energy in
$p\overline{p}$ Collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {19},
Pages = {191803},
Publisher = {American Physical Society},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.191803},
Abstract = {We present a search for a new particle T' decaying to a top
quark via T' → t + X, where X goes undetected. We use a
data sample corresponding to 5.7 fb(-1) of integrated
luminosity of p p collisions with sqrt[s] = 1.96 TeV,
collected at Fermilab Tevatron by the CDF II detector. Our
search for pair production of T' is focused on the hadronic
decay channel, pp → T'T' → tt + XX → bqq b qq + XX. We
interpret our results in terms of a model where T' is an
exotic fourth generation quark and X is a dark matter
particle. The data are consistent with standard model
expectations. We set a limit on the generic production of
T'T' → tt + XX, excluding the fourth generation exotic
quarks T' at 95% confidence level up to m(T') = 400 GeV/c(2)
for m(X) ≤ 70 GeV/c(2).},
Doi = {10.1103/PhysRevLett.107.191803},
Key = {fds308427}
}
@article{fds308484,
Author = {Aaltonen, and T, and others},
Title = {Search for New Bottomlike Quark Pair Decays $Q\bar{Q} \to
(tW^\mp)(\bar{t}W^\pm)$ in Same-Charge Dilepton
Events},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {9},
Pages = {091801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.091801},
Abstract = {http://arxiv.org/abs/0912.1057},
Doi = {10.1103/PhysRevLett.104.091801},
Key = {fds308484}
}
@article{fds308503,
Author = {Aaltonen, and T, and others},
Title = {Search for New Color-Octet Vector Particle Decaying to $t
\bar{t}$ in $p \bar{p}$ Collisions at $\sqrt{s}=1.96$
TeV},
Journal = {Phys. Lett.},
Volume = {B691},
Number = {4},
Pages = {183-190},
Publisher = {Elsevier BV},
Year = {2010},
url = {http://dx.doi.org/10.1016/j.physletb.2010.06.036},
Abstract = {http://arxiv.org/abs/0911.3112},
Doi = {10.1016/j.physletb.2010.06.036},
Key = {fds308503}
}
@article{fds308432,
Author = {Aaltonen, and T, and al, E},
Title = {Search for New Dielectron Resonances and {Randall-Sundrum}
Gravitons at the {Collider Detector at Fermilab}},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {5},
Pages = {051801},
Publisher = {American Physical Society},
Year = {2011},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.051801},
Abstract = {A search for new dielectron-mass resonances using data
recorded by the CDF II detector and corresponding to an
integrated luminosity of 5.7 fb(-1) is presented. No
significant excess over the expected standard model
prediction is observed. In this data set, an event with the
highest dielectron mass ever observed (960 GeV/c(2))
was recorded. The results are interpreted in the
Randall-Sundrum (RS) model. Combined with the
5.4 fb(-1) diphoton analysis, the RS-graviton
lower-mass limit for the coupling k/M¯(Pl)=0.1 is
1058 GeV/c(2), making it the strongest limit to
date.},
Doi = {10.1103/PhysRevLett.107.051801},
Key = {fds308432}
}
@article{fds308910,
Author = {al, FAE},
Title = {Search for new gauge bosons decaying into dielectrons in
(p)over-bar-p collisions at root-s=1.8 tev},
Journal = {Phys. Rev. D},
Volume = {51},
Number = {3},
Pages = {R949-R953},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevd.51.r949},
Abstract = {© 1995 The American Physical Society We have searched for
heavy neutral gauge bosons (Z') in p̄p collisions at s=1.8
TeV. The data were obtained using the CDF detector during
the 1992-1993 run corresponding to an integrated luminosity
of 19.7±0.7 pb-1. We present a 95% confidence level upper
limit on the production cross section times the branching
ratio of Z' decaying into dielectrons as a function of Z'
mass. Assuming standard model coupling strengths, we exclude
a Z' with a mass less than 505 GeV/c2. We also present lower
mass limits for Z' bosons from E6 models and the alternative
left-right model.},
Doi = {10.1103/physrevd.51.r949},
Key = {fds308910}
}
@article{fds308862,
Author = {al, FAE},
Title = {Search for new gauge bosons decaying into dileptons in
(p)over-bar-p collisions at root s=1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {79},
Number = {12},
Pages = {2192-2197},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.2192},
Abstract = {We have searched for heavy neutral gauge bosons (Z') in
dielectron and dimuon decay modes using 110pb-1 of p-p
collisions at √s = 1.8TeV collected with the Collider
Detector at Fermilab. We present a limit on the production
cross section times branching ratio of a Z' mass. For mass
MZ' > 600 GeV/c2, the upper limit is 40 fb at 95% confidence
level. We set the lower mass limits of 690, 590, 620, 595,
565, 630, and 600 GeV/c2 for Z'SM, ZΨ, Zψ, Zχ, ZI, ZLR,
and ZALRM, respectively. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.79.2192},
Key = {fds308862}
}
@article{fds308460,
Author = {Aaltonen, and T, and al, E},
Title = {Search for new heavy particles decaying to ${ZZ}\rightarrow
llll$, $lljj$ in $p\overline{p}$ collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {11},
Pages = {112008},
Publisher = {American Physical Society},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.83.112008},
Abstract = {We report on a search for anomalous production of Z boson
pairs through a massive resonance decay in data
corresponding to 2.5-2.9fb-1 of integrated luminosity in
pp̄ collisions at √s=1.96TeV using the CDF II detector at
the Fermilab Tevatron. This analysis, with more data and
channels where the Z bosons decay to muons or jets,
supersedes the 1.1fb-1 four-electron channel result
previously published by CDF. In order to maintain high
efficiency for muons, we use a new forward tracking
algorithm and muon identification requirements optimized for
these high signal-to-background channels. Predicting the
dominant backgrounds in each channel entirely from sideband
data samples, we observe four-body invariant mass spectra
above 300GeV/c2 that are consistent with background. We set
limits using the acceptance for a massive graviton resonance
that are 7-20 times stronger than the previously published
direct limits on resonant ZZ diboson production. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.83.112008},
Key = {fds308460}
}
@article{fds308768,
Author = {al, TAE},
Title = {Search for New Heavy Particles in the W Z0 Final State in pp
Collisions at $\sqrt{s} = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {88},
Number = {7},
Pages = {071806},
Year = {2002},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.88.071806},
Abstract = {The general search for new heavy particles, X, was
presented. The data collected by the Collider Detector at
Fermilab showed no evidence for production of X in 110 pb-1.
As a function of mass and width of new particle, the general
cross section limits were set at 95% C.L. An analysis of
results as mass limits on the production of new heavy
charged vector bosons was presented.},
Doi = {10.1103/physrevlett.88.071806},
Key = {fds308768}
}
@article{fds365421,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
Title = {Search for new non-resonant phenomena in high-mass dilepton
final states with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {11},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2020)005},
Abstract = {A search for new physics with non-resonant signals in
dielectron and dimuon final states in the mass range above 2
TeV is presented. This is the first search for non-resonant
signals in dilepton final states at the LHC to use a
background estimate from the data. The data, corresponding
to an integrated luminosity of 139 fb−1, were recorded by
the ATLAS experiment in proton-proton collisions at a
center-of-mass energy of s = 13 TeV during Run 2 of the
Large Hadron Collider. The benchmark signal signature is a
two-quark and two-lepton contact interaction, which would
enhance the dilepton event rate at the TeV mass scale. To
model the contribution from background processes a
functional form is fit to the dilepton invariant-mass
spectra in data in a mass region below the region of
interest. It is then extrapolated to a high-mass signal
region to obtain the expected background there. No
significant deviation from the expected background is
observed in the data. Upper limits at 95% CL on the number
of events and the visible cross-section times branching
fraction for processes involving new physics are provided.
Observed (expected) 95% CL lower limits on the contact
interaction energy scale reach 35.8 (37.6) TeV. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP11(2020)005},
Key = {fds365421}
}
@article{fds308800,
Author = {collaboration, CDF},
Title = {Search for New Particles Decaying to $t\bar{t}$ in
$p\bar{p}$ Collisions at $\sqrt{s}=1.8TeV$},
Journal = {Phys. Rev. Lett.},
Volume = {85},
Number = {2062},
Pages = {2062-2067},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://arXiv.org/ps/hep-ex/0003005},
Abstract = {http://arXiv.org/ps/hep-ex/0003005},
Doi = {10.1103/PhysRevLett.85.2062},
Key = {fds308800}
}
@article{fds308855,
Author = {al, FAE},
Title = {Search for new particles decaying into b(b)over-bar and
produced in association with W bosons decaying into e nu or
mu nu at the Fermilab Tevatron},
Journal = {Phys. Rev. Lett.},
Volume = {79},
Number = {20},
Pages = {3819-3824},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.3819},
Abstract = {We search for new particles that decay into b¯b and are
produced with W bosons in p¯p collisions at √s = 1.8TeV.
The search uses 109 ± 7pb-1 accumulated by the CDF
experiment at Fermilab. We select events with an eν or
μν, and two jets, one of them b tagged. The number of
events and the two-jet mass distribution are consistent with
expectations. Using W+Higgs production as a model for the
acceptance, we set an upper limit on the production cross
section times branching ratio for the new particle ranging
from 14 to 19 pb (95% C.L.) as the particle mass varies from
70 to 120GeV/c2. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.79.3819},
Key = {fds308855}
}
@article{fds308553,
Author = {Aaltonen, T and others},
Title = {Search for new particles decaying into dijets in
proton-antiproton collisions at sqrt(s) = 1.96
TeV},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {11},
Pages = {112002},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.112002},
Abstract = {We present a search for new particles which produce narrow
two-jet (dijet) resonances using proton-antiproton collision
data corresponding to an integrated luminosity of 1.13fb-1
collected with the CDFA II detector. The measured dijet mass
spectrum is found to be consistent with next-to-leading-order
perturbative QCD predictions, and no significant evidence of
new particles is found. We set upper limits at the 95%
confidence level on cross sections times the branching
fraction for the production of new particles decaying into
dijets with both jets having a rapidity magnitude |y| <1.
These limits are used to determine the mass exclusions for
the excited quark, axigluon, flavor-universal coloron, E6
diquark, color-octet techni-ρ, W′, and Z′. © 2009 The
American Physical Society.},
Doi = {10.1103/PhysRevD.79.112002},
Key = {fds308553}
}
@article{fds331645,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers,
W and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Culbertson, R and Dagenhart, D and Daniels, T and De Jongh and F and Dell’agnello, S},
Title = {Search for new particles decaying to b¯b in p¯p collisions
at √s=1.8TeV},
Journal = {Physical Review Letters},
Volume = {82},
Number = {10},
Pages = {2038-2043},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.2038},
Abstract = {We have used 87pb−1 of data collected with the collider
detector at Fermilab to search for new particles decaying to
b¯b. We present model-independent upper limits on the cross
section for narrow resonances which exclude the color-octet
technirho in the mass interval 350<M<440GeV/c2. In addition,
we exclude top-gluons, predicted in models of
top-color-assisted technicolor, of width Τ=0.3M in the mass
range 280<M<670GeV/c2, of width Τ=0.5M in the mass range
340<M<640GeV/c2, and of width Τ=0.7M in the mass range
375<M<560GeV/c2. © 1999 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.82.2038},
Key = {fds331645}
}
@article{fds308857,
Author = {al, FAE},
Title = {Search for new particles decaying to dijets at
CDF},
Journal = {Phys. Rev. D},
Volume = {55},
Number = {9},
Pages = {R5263-R5268},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.55.R5263},
Abstract = {We have used 106 pb[Formula presented] of data collected
with the Collider Detector at Fermilab to search for new
particles decaying to dijets. We exclude at the 95%
confidence level models containing the following new
particles: axigluons and flavor universal colorons with a
mass between 200 and 980 GeV/[Formula presented], excited
quarks with a mass between 80 and 570 GeV/[Formula
presented] and between 580 and 760 GeV/[Formula presented],
color octet techni-[Formula presented]’s with a mass
between 260 and 480 GeV/[Formula presented], [Formula
presented] bosons with a mass between 300 and 420
GeV/[Formula presented], and [Formula presented] diquarks
with a mass between 290 and 420 GeV/[Formula presented]. ©
1997 The American Physical Society.},
Doi = {10.1103/PhysRevD.55.R5263},
Key = {fds308857}
}
@article{fds308893,
Author = {al, FAE},
Title = {Search for new particles decaying to dijets in p(p)over-bar
collisions at root-s=1.8 tev},
Journal = {Phys. Rev. Lett.},
Volume = {74},
Number = {18},
Pages = {3538-3543},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevLett.74.3538},
Abstract = {We have used 19 pb-1 of data collected with the Collider
Detector at Fermilab to search for new particles decaying to
dijets. We exclude at 95% confidence level models containing
the following new particles: axigluons with mass between 200
and 870 GeV/ c2, excited quarks with mass between 80 and 570
GeV/ c2, and color octet technirhos with mass between 320
and 480 GeV/ c2. © 1995 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.74.3538},
Key = {fds308893}
}
@article{fds321333,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for new particles in events with one lepton and
missing transverse momentum in pp collisions at √s = 8 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {9},
Pages = {1-42},
Publisher = {Springer Nature},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2014)037},
Abstract = {This paper presents a search for new particles in events
with one lepton (electron or muon) and missing transverse
momentum using 20.3 fb−1 of proton-proton collision data
at √s = 8 TeV recorded by the ATLAS experiment at the
Large Hadron Collider. No significant excess beyond Standard
Model expectations is observed. A W ′ with Sequential
Standard Model couplings is excluded at the 95% confidence
level for masses up to 3.24 TeV. Excited chiral bosons (W*)
with equivalent coupling strengths are excluded for masses
up to 3.21 TeV. In the framework of an effective field
theory limits are also set on the dark matter-nucleon
scattering cross-section as well as the mass scale M* of the
unknown mediating interaction for dark matter pair
production in association with a leptonically decaying
W.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP09(2014)037},
Key = {fds321333}
}
@article{fds308638,
Author = {Aaltonen, and T, and others},
Title = {Search for New Particles Leading to $Z +$ jets Final States
in $p \bar{p}$ Collisions at $\sqrt{s}$ =
1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D76},
Number = {7},
Pages = {072006},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.76.072006},
Abstract = {We present the results of a search for new particles that
lead to a Z boson plus jets in p[overline p] collisions at
sqrt(s)=1.96 TeV using the Collider Detector at Fermilab
(CDF II). A data sample with a luminosity of 1.06 fb-1
collected using Z boson decays to ee and µµ is used. We
describe a completely data-based method to predict the
dominant background from standard model Z+jet events. This
method can be similarly applied to other analyses requiring
background predictions in multijet environments, as shown
when validating the method by predicting the background from
W+jets in t[overline t] production. No significant excess
above the background prediction is observed, and a limit is
set using a fourth generation quark model to quantify the
acceptance. Assuming BR(b[prime]-->bZ)=100\% and using a
leading-order calculation of the b[prime] cross section,
b[prime] quark masses below 268 GeV/c2 are excluded at 95%
confidence level.},
Doi = {10.1103/PhysRevD.76.072006},
Key = {fds308638}
}
@article{fds325884,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
Title = {Search for new phenomena in different-flavour high-mass
dilepton final states in pp collisions at [Formula:
see text] Tev with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {10},
Pages = {541},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4385-1},
Abstract = {A search is performed for a heavy particle decaying into
different flavour dilepton pairs ([Formula: see text],
[Formula: see text] or [Formula: see text]), using
3.2 fb[Formula: see text] of proton-proton collision data
at [Formula: see text] TeV collected in 2015 by the ATLAS
detector at the Large Hadron Collider. No excess over the
Standard Model prediction is observed. Limits at the 95 %
credibility level are set on the mass of a [Formula: see
text] boson with lepton-flavour-violating couplings at 3.0,
2.7 and 2.6 TeV, and on the mass of a supersymmetric
[Formula: see text] sneutrino with <i>R</i>-parity-violating
couplings at 2.3, 2.2 and 1.9 TeV, for [Formula: see text],
[Formula: see text] and [Formula: see text] final states,
respectively. The results are also interpreted as limits on
the threshold mass for quantum black hole
production.},
Doi = {10.1140/epjc/s10052-016-4385-1},
Key = {fds325884}
}
@article{fds321245,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
Title = {Search for New Phenomena in Dijet Angular Distributions in
Proton-Proton Collisions at sqrt[s]=8 TeV Measured with the
ATLAS Detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {22},
Pages = {221802},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.114.221802},
Abstract = {A search for new phenomena in LHC proton-proton collisions
at a center-of-mass energy of sqrt[s]=8 TeV was performed
with the ATLAS detector using an integrated luminosity of
17.3 fb^{-1}. The angular distributions are studied in
events with at least two jets; the highest dijet mass
observed is 5.5 TeV. All angular distributions are
consistent with the predictions of the standard model. In a
benchmark model of quark contact interactions, a
compositeness scale below 8.1 TeV in a destructive
interference scenario and 12.0 TeV in a constructive
interference scenario is excluded at 95% C.L.; median
expected limits are 8.9 TeV for the destructive interference
scenario and 14.1 TeV for the constructive interference
scenario.},
Doi = {10.1103/physrevlett.114.221802},
Key = {fds321245}
}
@article{fds321197,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Search for new phenomena in events with a photon and missing
transverse momentum in pp collisions at √s = 13 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {6},
Pages = {1-41},
Publisher = {Springer Nature},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2016)059},
Abstract = {Results of a search for new phenomena in events with an
energetic photon and large missing transverse momentum with
the ATLAS experiment at the Large Hadron Collider are
reported. The data were collected in proton-proton
collisions at a centre-of-mass energy of 13 TeV and
correspond to an integrated luminosity of 3.2 fb−1. The
observed data are in agreement with the Standard Model
expectations. Exclusion limits are presented in models of
new phenomena including pair production of dark matter
candidates or large extra spatial dimensions. In a
simplified model of dark matter and an axial-vector
mediator, the search excludes mediator masses below 710 GeV
for dark matter candidate masses below 150 GeV. In an
effective theory of dark matter production, values of the
suppression scale M∗ up to 570 GeV are excluded and the
effect of truncation for various coupling values is
reported. For the ADD large extra spatial dimension model
the search places more stringent limits than earlier
searches in the same event topology, excluding MD up to
about 2.3 (2.8) TeV for two (six) additional spatial
dimensions; the limits are reduced by 20-40% depending on
the number of additional spatial dimensions when applying a
truncation procedure.},
Doi = {10.1007/JHEP06(2016)059},
Key = {fds321197}
}
@article{fds321281,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for new phenomena in events with a photon and missing
transverse momentum in pp collisions at √s =8 TeV with the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.91.012008},
Abstract = {Results of a search for new phenomena in events with an
energetic photon and large missing transverse momentum with
the ATLAS experiment at the LHC are reported. Data were
collected in proton-proton collisions at a center-of-mass
energy of 8 TeV and correspond to an integrated luminosity
of 20.3 fb-1. The observed data are well described by the
expected Standard Model backgrounds. The expected (observed)
upper limit on the fiducial cross section for the production
of events with a photon and large missing transverse
momentum is 6.1 (5.3) fb at 95% confidence level. Exclusion
limits are presented on models of new phenomena with large
extra spatial dimensions, supersymmetric quarks, and direct
pair production of dark-matter candidates.},
Doi = {10.1103/PhysRevD.91.012008},
Key = {fds321281}
}
@article{fds315435,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP},
Title = {Search for new phenomena in events with at least three
photons collected in pp collisions at [Formula: see
text] = 8 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {4},
Pages = {210},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4034-8},
Abstract = {Results of a search for new phenomena in events with at
least three photons are reported. Data from proton-proton
collisions at a centre-of-mass energy of 8 TeV,
corresponding to an integrated luminosity of 20.3
fb[Formula: see text], were collected with the ATLAS
detector at the LHC. The observed data are well described by
the Standard Model. Limits at the 95 % confidence level on
new phenomena are presented based on the rate of events in
an inclusive signal region and a restricted signal region
targeting the rare decay [Formula: see text], as well as
di-photon and tri-photon resonance searches. For a Standard
Model Higgs boson decaying to four photons via a pair of
intermediate pseudoscalar particles (<i>a</i>), limits are
found to be [Formula: see text] for 10 GeV [Formula: see
text] 62 GeV. Limits are also presented for Higgs boson-like
scalars (<i>H</i>) for [Formula: see text] 125 GeV, and for
a [Formula: see text] decaying to three photons via
[Formula: see text]. Additionally, the observed limit on the
branching ratio of the <i>Z</i> boson decay to three photons
is found to be BR[Formula: see text], a result five times
stronger than the previous result from LEP.},
Doi = {10.1140/epjc/s10052-016-4034-8},
Key = {fds315435}
}
@article{fds308340,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for new phenomena in events with three charged
leptons at √s=7 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.87.052002},
Abstract = {A generic search for anomalous production of events with at
least three charged leptons is presented. The search uses a
pp-collision data sample at a center-of-mass energy of
√s=7 TeV corresponding to 4.6 fb-1 of integrated
luminosity collected in 2011 by the ATLAS detector at the
CERN Large Hadron Collider. Events are required to contain
at least two electrons or muons, while the third lepton may
either be an additional electron or muon, or a hadronically
decaying tau lepton. Events are categorized by the presence
or absence of a reconstructed tau-lepton or Z-boson
candidate decaying to leptons. No significant excess above
backgrounds expected from Standard Model processes is
observed. Results are presented as upper limits on event
yields from non-Standard-Model processes producing at least
three prompt, isolated leptons, given as functions of lower
bounds on several kinematic variables. Fiducial efficiencies
for model testing are also provided. The use of the results
is illustrated by setting upper limits on the production of
doubly charged Higgs bosons decaying to same-sign lepton
pairs.},
Doi = {10.1103/PhysRevD.87.052002},
Key = {fds308340}
}
@article{fds321235,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
M},
Title = {Search for new phenomena in events with three or more
charged leptons in pp collisions at √s=8 TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {8},
Publisher = {Springer Nature},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2015)138},
Abstract = {Abstract: A generic search for anomalous production of
events with at least three charged leptons is presented. The
data sample consists of pp collisions at √s=8 TeV
collected in 2012 by the ATLAS experiment at the CERN Large
Hadron Collider, and corresponds to an integrated luminosity
of 20.3 fb−1. Events are required to have at least three
selected lepton candidates, at least two of which must be
electrons or muons, while the third may be a hadronically
decaying tau. Selected events are categorized based on their
lepton flavour content and signal regions are constructed
using several kinematic variables of interest. No
significant deviations from Standard Model predictions are
observed. Model-independent upper limits on contributions
from beyond the Standard Model phenomena are provided for
each signal region, along with prescription to re-interpret
the limits for any model. Constraints are also placed on
models predicting doubly charged Higgs bosons and excited
leptons. For doubly charged Higgs bosons decaying to eτ or
μτ, lower limits on the mass are set at 400 GeV at 95%
confidence level. For excited leptons, constraints are
provided as functions of both the mass of the excited state
and the compositeness scale Λ, with the strongest mass
constraints arising in regions where the mass equals Λ. In
such scenarios, lower mass limits are set at 3.0 TeV for
excited electrons and muons, 2.5 TeV for excited taus, and
1.6 TeV for every excited-neutrino flavour.},
Doi = {10.1007/JHEP08(2015)138},
Key = {fds321235}
}
@article{fds365405,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for new phenomena in events with two opposite-charge
leptons, jets and missing transverse momentum in pp
collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2021)165},
Abstract = {The results of a search for direct pair production of top
squarks and for dark matter in events with two
opposite-charge leptons (electrons or muons), jets and
missing transverse momentum are reported, using 139 fb−1
of integrated luminosity from proton-proton collisions at s
= 13 TeV, collected by the ATLAS detector at the Large
Hadron Collider during Run 2 (2015–2018). This search
considers the pair production of top squarks and is
sensitive across a wide range of mass differences between
the top squark and the lightest neutralino. Additionally,
spin-0 mediator dark-matter models are considered, in which
the mediator is produced in association with a pair of top
quarks. The mediator subsequently decays to a pair of
dark-matter particles. No significant excess of events is
observed above the Standard Model background, and limits are
set at 95% confidence level. The results exclude top squark
masses up to about 1 TeV, and masses of the lightest
neutralino up to about 500 GeV. Limits on dark-matter
production are set for scalar (pseudoscalar) mediator masses
up to about 250 (300) GeV. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP04(2021)165},
Key = {fds365405}
}
@article{fds308406,
Author = {Kotwal, AV and Collaboration, CDF},
Title = {Search for new phenomena in events with two Z bosons and
missing transverse momentum in ppbar collisions at
sqrt(s)=1.96 TeV},
Journal = {Phys. Rev. D},
Volume = {85},
Number = {1},
Pages = {011104(R)},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.011104},
Abstract = {We present a search for new phenomena in events with two
reconstructed Z bosons and large missing transverse
momentum, sensitive to processes pp̄→X 2X 2→ZZX 1X 1,
where X 2 is an unstable particle decaying as X 2→ ZX 1
and X 1 is undetected. The particles X 1 and X 2 may be,
among other possibilities, fourth-generation neutrinos or
supersymmetric particles. We study the final state in which
one Z boson decays to two charged leptons and the second
decays hadronically. In data corresponding to an integrated
luminosity of 4.2fb -1 from proton-antiproton collisions
recorded by the CDF II detector at the Tevatron, with
center-of-mass energy of 1.96 TeV, we find agreement between
data and standard-model backgrounds. We calculate 95%
confidence level upper limits on the cross section of the
process pp̄→X 2X 2→ZZX 1X 1 ranging from 50 fb to 1 pb,
depending on the masses of X 1 and X 2. © 2012 American
Physical Society.},
Doi = {10.1103/PhysRevD.85.011104},
Key = {fds308406}
}
@article{fds321298,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
C},
Title = {Search for new phenomena in final states with an energetic
jet and large missing transverse momentum in pp
collisions at [Formula: see text]TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {299},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3517-3},
Abstract = {Results of a search for new phenomena in final states with
an energetic jet and large missing transverse momentum are
reported. The search uses 20.3 fb[Formula: see text] of
[Formula: see text] TeV data collected in 2012 with the
ATLAS detector at the LHC. Events are required to have at
least one jet with [Formula: see text] GeV and no leptons.
Nine signal regions are considered with increasing missing
transverse momentum requirements between [Formula: see
text] GeV and [Formula: see text] GeV. Good agreement is
observed between the number of events in data and Standard
Model expectations. The results are translated into
exclusion limits on models with either large extra spatial
dimensions, pair production of weakly interacting dark
matter candidates, or production of very light gravitinos in
a gauge-mediated supersymmetric model. In addition, limits
on the production of an invisibly decaying Higgs-like boson
leading to similar topologies in the final state are
presented.},
Doi = {10.1140/epjc/s10052-015-3517-3},
Key = {fds321298}
}
@article{fds321181,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for new phenomena in final states with an energetic
jet and large missing transverse momentum in pp collisions
at s =13 TeV using the ATLAS detector},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.032005},
Abstract = {Results of a search for new phenomena in final states with
an energetic jet and large missing transverse momentum are
reported. The search uses proton-proton collision data
corresponding to an integrated luminosity of 3.2 fb-1 at
s=13 TeV collected in 2015 with the ATLAS detector at the
Large Hadron Collider. Events are required to have at least
one jet with a transverse momentum above 250 GeV and no
leptons. Several signal regions are considered with
increasing missing-transverse-momentum requirements between
ETmiss>250 GeV and ETmiss>700 GeV. Good agreement is
observed between the number of events in data and Standard
Model predictions. The results are translated into exclusion
limits in models with large extra spatial dimensions, pair
production of weakly interacting dark-matter candidates, and
the production of supersymmetric particles in several
compressed scenarios.},
Doi = {10.1103/PhysRevD.94.032005},
Key = {fds321181}
}
@article{fds365400,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arguin, JF and Argyropoulos,
S},
Title = {Search for new phenomena in final states with b-jets and
missing transverse momentum in √s = 13 TeV pp collisions
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {5},
Year = {2021},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2021)093},
Abstract = {The results of a search for new phenomena in final states
with b-jets and missing transverse momentum using 139 fb−1
of proton-proton data collected at a centre-of-mass energy s
= 13 TeV by the ATLAS detector at the LHC are reported. The
analysis targets final states produced by the decay of a
pair-produced supersymmetric bottom squark into a bottom
quark and a stable neutralino. The analysis also seeks
evidence for models of pair production of dark matter
particles produced through the decay of a generic scalar or
pseudoscalar mediator state in association with a pair of
bottom quarks, and models of pair production of scalar
third-generation down-type leptoquarks. No significant
excess of events over the Standard Model background
expectation is observed in any of the signal regions
considered by the analysis. Bottom squark masses below 1270
GeV are excluded at 95% confidence level if the neutralino
is massless. In the case of nearly mass-degenerate bottom
squarks and neutralinos, the use of dedicated
secondary-vertex identification techniques permits the
exclusion of bottom squarks with masses up to 660 GeV for
mass splittings between the squark and the neutralino of 10
GeV. These limits extend substantially beyond the regions of
parameter space excluded by similar ATLAS searches performed
previously. [Figure not available: see fulltext.]},
Doi = {10.1007/JHEP05(2021)093},
Key = {fds365400}
}
@article{fds308309,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Search for new phenomena in final states with large jet
multiplicities and missing transverse momentum at √s = 8
TeV proton-proton collisions using the ATLAS
experiment},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {10},
Publisher = {Springer Nature},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2013)130},
Abstract = {A search is presented for new particles decaying to large
numbers (7 or more) of jets, with missing transverse
momentum and no isolated electrons or muons. This analysis
uses 20:3 fb-1 of pp collision data at √s = 8 TeV
collected by the ATLAS experiment at the Large Hadron
Collider. The sensitivity of the search is enhanced by
considering the number of b-tagged jets and the scalar sum
of masses of large-radius jets in an event. No evidence is
found for physics beyond the Standard Model. The results are
interpreted in the context of various simplified
supersymmetry-inspired models where gluinos are pair
produced, as well as an mSUGRA/CMSSM model. © SISSA
2013.},
Doi = {10.1007/JHEP10(2013)130},
Key = {fds308309}
}
@article{fds314850,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A},
Title = {Search for new phenomena in final states with large jet
multiplicities and missing transverse momentum with ATLAS
using √s=13 TeV proton–proton collisions},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {757},
Pages = {334-355},
Publisher = {Elsevier BV},
Year = {2016},
Month = {June},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2016.04.005},
Abstract = {Results are reported of a search for new phenomena, such as
supersymmetric particle production, that could be observed
in high-energy proton–proton collisions. Events with large
numbers of jets, together with missing transverse momentum
from unobserved particles, are selected. The data analysed
were recorded by the ATLAS experiment during 2015 using the
13 TeV centre-of-mass proton–proton collisions at the
Large Hadron Collider, and correspond to an integrated
luminosity of 3.2 fb−1. The search selected events with
various jet multiplicities from ≥7 to ≥10 jets, and with
various b-jet multiplicity requirements to enhance
sensitivity. No excess above Standard Model expectations is
observed. The results are interpreted within two
supersymmetry models, where gluino masses up to 1400 GeV are
excluded at 95% confidence level, significantly extending
previous limits.},
Doi = {10.1016/j.physletb.2016.04.005},
Key = {fds314850}
}
@article{fds308288,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Search for new phenomena in photon + jet events collected in
proton-proton collisions at √s = 8 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {728},
Number = {1},
Pages = {562-578},
Publisher = {Elsevier BV},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2013.12.029},
Abstract = {This Letter describes a model-independent search for the
production of new resonances in photon + jet (γ + jet)
events using 20 fb-1 of proton-proton LHC data recorded with
the ATLAS detector at a centre-of-mass energy of √s = 8
TeV. The γ + jet mass distribution is compared to a
background model fit from data; no significant deviation
from the background-only hypothesis is found. Limits are set
at 95% credibility level on generic Gaussian-shaped signals
and two benchmark phenomena beyond the Standard Model:
non-thermal quantum black holes and excited quarks.
Non-thermal quantum black holes are excluded below masses of
4.6 TeV and excited quarks are excluded below masses of 3.5
TeV. © 2013 The Authors. Published by Elsevier
B.V.},
Doi = {10.1016/j.physletb.2013.12.029},
Key = {fds308288}
}
@article{fds321263,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for new phenomena in the dijet mass distribution
using pp collision data at √s =8 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.91.052007},
Abstract = {Dijet events produced in LHC proton-proton collisions at a
center-of-mass energy s=8 TeV are studied with the ATLAS
detector using the full 2012 data set, with an integrated
luminosity of 20.3 fb-1. Dijet masses up to about 4.5 TeV
are probed. No resonancelike features are observed in the
dijet mass spectrum. Limits on the cross section times
acceptance are set at the 95% credibility level for various
hypotheses of new phenomena in terms of mass or energy
scale, as appropriate. This analysis excludes excited quarks
with a mass below 4.06 TeV, color-octet scalars with a mass
below 2.70 TeV, heavy W′ bosons with a mass below 2.45
TeV, chiral W∗ bosons with a mass below 1.75 TeV, and
quantum black holes with six extra space-time dimensions
with threshold mass below 5.66 TeV.},
Doi = {10.1103/PhysRevD.91.052007},
Key = {fds321263}
}
@article{fds376251,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena,
E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis,
K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian,
R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio,
EL and Barberis, D and Barbero, M and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau,
T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry,
T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac,
D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold,
T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély,
AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov,
G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruni,
A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr,
JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev, AR and Cabrera
Urbán, S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson,
EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter,
JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli,
A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chan,
J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM},
Title = {Search for New Phenomena in Two-Body Invariant Mass
Distributions Using Unsupervised Machine Learning for
Anomaly Detection at sqrt[s]=13 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {132},
Number = {8},
Pages = {081801},
Year = {2024},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.132.081801},
Abstract = {Searches for new resonances are performed using an
unsupervised anomaly-detection technique. Events with at
least one electron or muon are selected from
140 fb^{-1} of pp collisions at sqrt[s]=13 TeV
recorded by ATLAS at the Large Hadron Collider. The approach
involves training an autoencoder on data, and subsequently
defining anomalous regions based on the reconstruction loss
of the decoder. Studies focus on nine invariant mass spectra
that contain pairs of objects consisting of one light jet or
b jet and either one lepton (e,μ), photon, or second light
jet or b jet in the anomalous regions. No significant
deviations from the background hypotheses are observed.
Limits on contributions from generic Gaussian signals with
various widths of the resonance mass are obtained for nine
invariant masses in the anomalous regions.},
Doi = {10.1103/physrevlett.132.081801},
Key = {fds376251}
}
@article{fds365406,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for new phenomena with top quark pairs in final
states with one lepton, jets, and missing transverse
momentum in pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2021)174},
Abstract = {A search for new phenomena with top quark pairs in final
states with one isolated electron or muon, multiple jets,
and large missing transverse momentum is performed. Signal
regions are designed to search for two-, three-, and
four-body decays of the directly pair-produced
supersymmetric partner of the top quark (stop). Additional
signal regions are designed specifically to search for
spin-0 mediators that are produced in association with a
pair of top quarks and decay into a pair of dark-matter
particles. The search is performed using the Large Hadron
Collider proton-proton collision dataset at a centre-of-mass
energy of s = 13 TeV recorded by the ATLAS detector from
2015 to 2018, corresponding to an integrated luminosity of
139 fb−1. No significant excess above the Standard Model
background is observed, and limits at 95% confidence level
are set in the stop-neutralino mass plane and as a function
of the mediator mass or the dark-matter particle mass. Stops
are excluded up to 1200 GeV (710 GeV) in the two-body
(three-body) decay scenario. In the four-body scenario stops
up to 640 GeV are excluded for a stop-neutralino mass
difference of 60 GeV. Scalar and pseudoscalar dark-matter
mediators are excluded up to 200 GeV when the coupling
strengths of the mediator to Standard Model and dark-matter
particles are both equal to one and when the mass of the
dark-matter particle is 1 GeV. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP04(2021)174},
Key = {fds365406}
}
@article{fds308428,
Author = {Aaltonen, TEA},
Title = {Search for New Physics in High ${p}_{T}$ Like-Sign Dilepton
Events at {CDF II}},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {18},
Pages = {181801},
Publisher = {American Physical Society},
Year = {2011},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.181801},
Abstract = {We present a search for new physics in events with two high
pT leptons of the same electric charge, using data with an
integrated luminosity of 6.1 fb(-1). The observed data are
consistent with standard model predictions. We set 95% C.L.
lower limits on the mass of doubly charged scalars decaying
to like-sign dileptons, m(H±±) > 190-245 GeV/c(2),
assuming 100% BR to ee, μμ or eμ.},
Doi = {10.1103/PhysRevLett.107.181801},
Key = {fds308428}
}
@article{fds308621,
Author = {Aaltonen, and T, and others},
Title = {Search for new physics in high mass electron-positron events
in $p \bar{p}$ collisions at $\sqrt{s}$ =
1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {17},
Pages = {171802},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.171802},
Abstract = {We report the results of a search for a narrow resonance in
electron-positron events in the invariant mass range of
150--950 GeV/c2 using 1.3 fb-1 of p[overline p] collision
data at sqrt(s)=1.96 TeV collected by the CDF II detector at
Fermilab. No significant evidence of such a resonance is
observed and we interpret the results to exclude the
standard-model-like Z[prime] with a mass below 923 GeV/c2
and the Randall-Sundrum graviton with a mass below 807
GeV/c2 for k/[overline M]pl=0.1, both at the 95\% confidence
level. Combining with diphoton data excludes the
Randall-Sundrum graviton for masses below 889 GeV/c2 for
k/[overline M]pl=0.1.},
Doi = {10.1103/physrevlett.99.171802},
Key = {fds308621}
}
@article{fds308660,
Author = {Abulencia, and A, and others},
Title = {Search for new physics in lepton + photon + X events with
305-pb**(-1) of p anti-p collisions at s**(1/2) = 1.96-
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {97},
Number = {3},
Pages = {031801},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.97.031801},
Abstract = {We present results of a search for anomalous production of
events containing a charged lepton (either electron or muon)
and a photon, both with high transverse momentum,
accompanied by additional signatures, X, including missing
transverse energy (MET) and additional leptons and photons.
We use the same kinematic selection criteria as in a
previous CDF search, but with a substantially larger data
set, 305 pb-1, a ppbar collision energy of 1.96 TeV, and the
upgraded CDF II detector. We find 42 Lepton+Photon+MET
events versus a standard model expectation of 37.3 +- 5.4
events. The level of excess observed in Run I, 16 events
with an expectation of 7.6 +- 0.7 events (corresponding to a
2.7 sigma effect), is not supported by the new data. In the
signature of Multi-Lepton+Photon+X we observe 31 events
versus an expectation of 23.0 +- 2.7 events. In this sample
we find no events with an extra photon or MET and so find no
events like the one ee+gg+MET event observed in Run
I.},
Doi = {10.1103/physrevlett.97.031801},
Key = {fds308660}
}
@article{fds308757,
Author = {al, DAE},
Title = {Search for New Physics in Photon-Lepton Events in pp
Collisions at $\sqrt{s} = 1.8TeV,},
Journal = {Physical Review Letters},
Volume = {89},
Number = {4},
Pages = {041802},
Year = {2002},
url = {http://dx.doi.org/10.1103/physrevlett.89.041802},
Abstract = {We present the results of a search in pp collisions at
sqrt[s] = 1.8 TeV for anomalous production of events
containing a photon and a lepton (e or mu), both with large
transverse energy, using 86 pb(-1) of data collected with
the Collider Detector at Fermilab during the 1994-1995
collider run at the Fermilab Tevatron. The presence of large
missing transverse energy (E(T)), additional photons, or
additional leptons in these events is also analyzed. The
results are consistent with standard model expectations,
with the possible exception of photon-lepton events with
large E(T), for which the observed total is 16 events and
the expected mean total is 7.6+/-0.7 events.},
Doi = {10.1103/physrevlett.89.041802},
Key = {fds308757}
}
@article{fds308761,
Author = {Acosta, D and Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, M and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D},
Title = {Search for new physics in photon-lepton events in [Formula
Presented] collisions at [Formula Presented]},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {66},
Number = {1},
Pages = {120041-1200427},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.66.012004},
Abstract = {We present the results of a search in [Formula Presented]
collisions at [Formula Presented] for anomalous production
of events containing a photon with large transverse energy
and a lepton [Formula Presented] or [Formula Presented] with
large transverse energy, using [Formula Presented] of data
collected with the Collider Detector at Fermilab during the
1994–1995 collider run at the Fermilab Tevatron. The
presence of large missing transverse energy [Formula
Presented] additional photons, or additional leptons in
these events is also analyzed. The results are consistent
with standard model expectations, with the possible
exception of photon-lepton events with large [Formula
Presented] for which the observed total is 16 events and the
expected mean total is [Formula Presented] events. © 2002
The American Physical Society.},
Doi = {10.1103/PhysRevD.66.012004},
Key = {fds308761}
}
@article{fds308544,
Author = {Aaltonen, T and others},
Title = {Search for new physics in the mu mu + e/mu + E-slash [sub T]
channel with a low-p[sub T] lepton threshold at the Collider
Detector at Fermilab},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {5},
Pages = {052004},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.052004},
Abstract = {A search for new physics using three-lepton (trilepton) data
collected with the CDF II detector and corresponding to an
integrated luminosity of 976 pb-1 is presented. The standard
model predicts a low rate of trilepton events, which makes
some supersymmetric processes, such as chargino-neutralino
production, measurable in this channel. The μμ+ signature
is investigated, where ℓ is an electron or a muon, with
the additional requirement of large missing transverse
energy. In this analysis, the lepton transverse momenta with
respect to the beam direction (pT) are as low as 5GeV/c, a
selection that improves the sensitivity to particles that
are light as well as to ones that result in leptonically
decaying tau leptons. At the same time, this low-pT
selection presents additional challenges due to the
non-negligible heavy-quark background at low lepton momenta.
This background is measured with an innovative technique
using experimental data. Several dimuon and trilepton
control regions are investigated, and good agreement between
experimental results and standard-model predictions is
observed. In the signal region, we observe one three-muon
event and expect 0.4±0.1μμ+ events from standard-model
processes. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevD.79.052004},
Key = {fds308544}
}
@article{fds321613,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Search for new physics in trilepton events and limits on the
associated chargino-neutralino production at
CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {1},
Pages = {012011},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.90.012011},
Abstract = {We perform a search for new physics using final states
consisting of three leptons and a large imbalance in
transverse momentum resulting from proton-antiproton
collisions at 1.96 TeV center-of-mass energy. We use data
corresponding to 5.8fb-1 of integrated luminosity recorded
by the CDF II detector at the Tevatron collider. Our main
objective is to investigate possible new low-momentum (down
to 5GeV/c) multileptonic final states not investigated by
LHC experiments. Relative to previous CDF analyses, we
expand the geometric and kinematic coverage of electrons and
muons and utilize tau leptons that decay hadronically.
Inclusion of tau leptons is particularly important for
supersymmetry (SUSY) searches. The results are consistent
with standard-model predictions within 1.85σ. By optimizing
our event selection to increase sensitivity to the minimal
supergravity (mSUGRA) SUSY model, we set limits on the
associated production of chargino and next-to-lightest
neutralino, the SUSY partners of the electroweak gauge
bosons. We exclude cross sections up to 0.1 pb and chargino
masses up to 168GeV/c2 at 95% C.L., for a suitable set of
mSUGRA parameters. We also exclude a region of the
two-dimensional space of the masses of the neutralino and
the supersymmetric partner of the tau lepton, not previously
excluded at the Tevatron. © 2014 American Physical
Society.},
Doi = {10.1103/PhysRevD.90.012011},
Key = {fds321613}
}
@article{fds308471,
Author = {Aaltonen, and T, and others},
Title = {Search for New Physics with a Dijet Plus Missing $E_{T}$
Signature in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
Collisions at $\sqrt{s}=1.96\,\,TeV$},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {13},
Pages = {131801},
Publisher = {American Physical Society},
Year = {2010},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.131801},
Abstract = {We present results of a signature-based search for new
physics using a dijet plus missing transverse energy (E(T))
data sample collected in 2 fb⁻¹ of pp collisions at
√s=1.96 TeV with the CDF II detector at the Fermilab
Tevatron. We observe no significant event excess with
respect to the standard model prediction and extract a 95%
C.L. upper limit on the cross section times acceptance for a
potential contribution from a nonstandard model process. The
search is made by using novel, data-driven techniques for
estimating backgrounds that are applicable to first searches
at the LHC.},
Doi = {10.1103/PhysRevLett.105.131801},
Key = {fds308471}
}
@article{fds321146,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for new resonances in events with one lepton and
missing transverse momentum in pp collisions at √s=13 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {762},
Pages = {334-352},
Publisher = {Elsevier BV},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2016.09.040},
Abstract = {A search for W′ bosons in events with one lepton (electron
or muon) and missing transverse momentum is presented. The
search uses 3.2 fb−1 of pp collision data collected at
s=13 TeV by the ATLAS experiment at the LHC in 2015. The
transverse mass distribution is examined and no significant
excess of events above the level expected from Standard
Model processes is observed. Upper limits on the W′ boson
cross-section times branching ratio to leptons are set as a
function of the W′ mass. Within the Sequential Standard
Model W′ masses below 4.07 TeV are excluded at the 95%
confidence level. This extends the limit set using LHC data
at s=8 TeV by around 800 GeV.},
Doi = {10.1016/j.physletb.2016.09.040},
Key = {fds321146}
}
@article{fds321314,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for new resonances in Wγ and Zγ final states in pp
collisions at √s=8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {738},
Pages = {428-447},
Publisher = {Elsevier BV},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2014.10.002},
Abstract = {This letter presents a search for new resonances decaying to
final states with a vector boson produced in association
with a high transverse momentum photon, Vγ with
V=W(→ℓν) or Z(→ℓ+ℓ−), where ℓ=e or μ. The
measurements use 20.3 fb−1 of proton–proton collision
data at a center–of–mass energy of s=8 TeV recorded with
the ATLAS detector. No deviations from the Standard Model
expectations are found, and production cross section limits
are set at 95% confidence level. Masses of the hypothetical
aT and ωT states of a benchmark Low Scale Technicolor model
are excluded in the ranges [275,960] GeV and
[200,700]∪[750,890] GeV, respectively. Limits at 95%
confidence level on the production cross section of a
singlet scalar resonance decaying to Zγ final states have
also been obtained for masses below 1180
GeV.},
Doi = {10.1016/j.physletb.2014.10.002},
Key = {fds321314}
}
@article{fds375880,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Search for non-resonant production of semi-visible jets
using Run 2 data in ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {848},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138324},
Abstract = {Semi-visible jets, with a significant contribution to the
event's missing transverse momentum, can arise in strongly
interacting dark sectors. This results in an event topology
where one of the jets can be aligned with the direction of
the missing transverse momentum. The first search for
semi-visible jets produced via a t-channel mediator exchange
is presented. The analysis uses proton-proton collisions
with an integrated luminosity of 139 fb−1 and a
centre-of-mass energy of 13 TeV, collected with the ATLAS
detector during the Run 2 of the LHC. No excess over
Standard Model predictions is observed. Assuming a coupling
strength of unity between the mediator, a Standard Model
quark and a dark quark, mediator masses up to 2.7 TeV are
excluded at the 95% confidence level. Upper limits on the
coupling strength are also derived.},
Doi = {10.1016/j.physletb.2023.138324},
Key = {fds375880}
}
@article{fds321309,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F},
Title = {Search for nonpointing and delayed photons in the diphoton
and missing transverse momentum final state in 8 TeV pp
collisions at the LHC using the ATLAS detector SEARCH for
NONPOINTING and DELAYED PHOTONS in ⋯ G. AAD et
al.},
Journal = {Zeitschrift fur Antikes Christentum},
Volume = {19},
Number = {3},
Pages = {1DUMMY},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.90.112005},
Abstract = {© 2014 CERN. © 2014 CERN, for the ATLAS Collaboration.
Published by the American Physical Society under the terms
of the »http://creativecommons.org/licenses/by/3.0/»
Creative Commons Attribution 3.0 License. Further
distribution of this work must maintain attribution to the
author(s) and the published article's title, journal
citation, and DOI.A search has been performed, using the
full 20.3 fb-1 data sample of 8 TeV proton-proton collisions
collected in 2012 with the ATLAS detector at the LHC, for
photons originating from a displaced vertex due to the decay
of a neutral long-lived particle into a photon and an
invisible particle. The analysis investigates the diphoton
plus missing transverse momentum final state, and is
therefore most sensitive to pair production of long-lived
particles. The analysis technique exploits the capabilities
of the ATLAS electromagnetic calorimeter to make precise
measurements of the flight direction, as well as the time of
flight, of photons. No excess is observed over the Standard
Model predictions for background. Exclusion limits are set
within the context of gauge mediated supersymmetry breaking
models, with the lightest neutralino being the
next-to-lightest supersymmetric particle and decaying into a
photon and gravitino with a lifetime in the range from 250
ps to about 100 ns.},
Doi = {10.1103/PhysRevD.90.112005},
Key = {fds321309}
}
@article{fds308323,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Search for nonpointing photons in the diphoton and ETmiss
final state in √s=7 TeV proton-proton collisions using the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.88.012001},
Abstract = {A search has been performed for photons originating in the
decay of a neutral long-lived particle, exploiting the
capabilities of the ATLAS electromagnetic calorimeter to
make precise measurements of the flight direction of
photons, as well as the calorimeter's excellent time
resolution. The search has been made in the diphoton plus
missing transverse energy final state, using the full data
sample of 4.8 fb-1 of 7 TeV proton-proton collisions
collected in 2011 with the ATLAS detector at the LHC. No
excess is observed above the background expected from
Standard Model processes. The results are used to set
exclusion limits in the context of gauge mediated
supersymmetry breaking models, with the lightest neutralino
being the next-to-lightest supersymmetric particle and
decaying with a lifetime in excess of 0.25 ns into a photon
and a gravitino. © 2013 CERN.},
Doi = {10.1103/PhysRevD.88.012001},
Key = {fds308323}
}
@article{fds375909,
Author = {Amerl, M and Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori, G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang,
R and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Ghosh, A and Johns,
KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK},
Title = {Search for nonresonant pair production of Higgs bosons in
the bb¯bb¯ final state in pp collisions at √s = 13 TeV
with the ATLAS detector},
Journal = {Physical Review D},
Volume = {108},
Number = {5},
Year = {2023},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.108.052003},
Abstract = {A search for nonresonant Higgs boson pair production in the
Formula Presented final state is presented. The analysis
uses Formula Presented of Formula Presented collision data
at Formula Presented collected with the ATLAS detector at
the Large Hadron Collider, and targets both the gluon-gluon
fusion and vector-boson fusion production modes. No evidence
of the signal is found and the observed (expected) upper
limit on the cross section for nonresonant Higgs boson pair
production is determined to be 5.4 (8.1) times the Standard
Model predicted cross section at 95% confidence level.
Constraints are placed on modifiers to the Formula Presented
and Formula Presented couplings. The observed (expected)
Formula Presented constraints on the Formula Presented
coupling modifier, Formula Presented, are determined to be
Formula Presented (Formula Presented), while the
corresponding constraints for the Formula Presented coupling
modifier, Formula Presented, are Formula Presented (Formula
Presented). In addition, constraints on relevant
coefficients are derived in the context of the Standard
Model effective field theory and Higgs effective field
theory, and upper limits on the Formula Presented production
cross section are placed in seven Higgs effective field
theory benchmark scenarios.},
Doi = {10.1103/PhysRevD.108.052003},
Key = {fds375909}
}
@article{fds321317,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for pair and single production of new heavy quarks
that decay to a Z boson and a third-generation quark in pp
collisions at √ S = 8TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {11},
Publisher = {Springer Nature},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2014)104},
Abstract = {Abstract: A search is presented for the production of new
heavy quarks that decay to a Z boson and a third-generation
Standard Model quark. In the case of a new charge +2/3 quark
(T ), the decay targeted is T → Zt, while the decay
targeted for a new charge −1/3 quark (B) is B → Zb. The
search is performed with a dataset corresponding to 20.3
fb−1 of pp collisions at (Formula presented.) TeV recorded
in 2012 with the ATLAS detector at the CERN Large Hadron
Collider. Selected events contain a high transverse momentum
Z boson candidate reconstructed from a pair of oppositely
charged same-flavor leptons (electrons or muons), and are
analyzed in two channels defined by the absence or presence
of a third lepton. Hadronic jets, in particular those with
properties consistent with the decay of a b-hadron, are also
required to be present in selected events. Different
requirements are made on the jet activity in the event in
order to enhance the sensitivity to either heavy quark pair
production mediated by the strong interaction, or single
production mediated by the electroweak interaction. No
significant excess of events above the Standard Model
expectation is observed, and lower limits are derived on the
mass of vector-like T and B quarks under various branching
ratio hypotheses, as well as upper limits on the magnitude
of electroweak coupling parameters.},
Doi = {10.1007/JHEP11(2014)104},
Key = {fds321317}
}
@article{fds321216,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Search for pair production of a new heavy quark that decays
into a W boson and a light quark in pp collisions at s =8
TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.92.112007},
Abstract = {A search is presented for pair production of a new heavy
quark (Q) that decays into a W boson and a light quark (q)
in the final state where one W boson decays leptonically (to
an electron or muon plus a neutrino) and the other W boson
decays hadronically. The analysis is performed using an
integrated luminosity of 20.3 fb-1 of pp collisions at s=8
TeV collected by the ATLAS detector at the LHC. No evidence
of QQ¯ production is observed. New chiral quarks with
masses below 690 GeV are excluded at 95% confidence level,
assuming BR(Q→Wq)=1. Results are also interpreted in the
context of vectorlike quark models, resulting in the limits
on the mass of a vectorlike quark in the two-dimensional
plane of BR(Q→Wq) versus BR(Q→Hq).},
Doi = {10.1103/PhysRevD.92.112007},
Key = {fds321216}
}
@article{fds321182,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
A},
Title = {Search for pair production of gluinos decaying via stop and
sbottom in events with b -jets and large missing transverse
momentum in pp collisions at s =13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.032003},
Abstract = {A search for supersymmetry involving the pair production of
gluinos decaying via third-generation squarks to the
lightest neutralino (χ10) is reported. It uses an LHC
proton-proton data set at a center-of-mass energy s=13 TeV
with an integrated luminosity of 3.2 fb-1 collected with the
ATLAS detector in 2015. The signal is searched for in events
containing several energetic jets, of which at least three
must be identified as b jets, large missing transverse
momentum, and, potentially, isolated electrons or muons.
Large-radius jets with a high mass are also used to identify
highly boosted top quarks. No excess is found above the
predicted background. For χ10 masses below approximately
700 GeV, gluino masses of less than 1.78 TeV and 1.76 TeV
are excluded at the 95% C.L. in simplified models of the
pair production of gluinos decaying via sbottom and stop,
respectively. These results significantly extend the
exclusion limits obtained with the s=8 TeV data
set.},
Doi = {10.1103/PhysRevD.94.032003},
Key = {fds321182}
}
@article{fds308353,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
Costa, JJBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Bege, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Busey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, JJ and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas,
CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, JJ and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A},
Title = {Search for pair production of heavy top-like quarks decaying
to a high-pT W boson and a b
quark in the lepton plus jets final state at √s=7
TeV with the ATLAS detector},
Journal = {PHYSICS LETTERS B},
Volume = {718},
Number = {4-5},
Pages = {1284-1302},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2012.11.071},
Abstract = {© 2012 CERN A search is presented for production of a heavy
up-type quark (t′) together with its antiparticle,
assuming a significant branching ratio for subsequent decay
into a W boson and a b quark. The search is based on 4.7
fb−1 of pp collisions at s=7 TeV recorded in 2011 with the
ATLAS detector at the CERN Large Hadron Collider. Data are
analyzed in the lepton + jets final state, characterized by
a high-transverse-momentum isolated electron or muon, large
missing transverse momentum and at least three jets. The
analysis strategy relies on the substantial boost of the W
bosons in the t′t¯′ signal when mt′≳400 GeV. No
significant excess of events above the Standard Model
expectation is observed and the result of the search is
interpreted in the context of fourth-generation and
vector-like quark models. Under the assumption of a
branching ratio BR(t′→Wb)=1, a fourth-generation t′
quark with mass lower than 656 GeV is excluded at 95%
confidence level. In addition, in light of the recent
discovery of a new boson of mass ∼126 GeV at the LHC,
upper limits are derived in the two-dimensional plane of
BR(t′→Wb) versus BR(t′→Ht), where H is the Standard
Model Higgs boson, for vector-like quarks of various
masses.},
Doi = {10.1016/j.physletb.2012.11.071},
Key = {fds308353}
}
@article{fds321172,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for pair production of Higgs bosons in the bbbb final
state using proton-proton collisions at √s =13 TeV with
the ATLAS detector},
Journal = {Physical Review D},
Volume = {94},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.94.052002},
Abstract = {A search for Higgs-boson pair production in the bbbb final
state is carried out with 3.2 fb-1 of proton-proton
collision data collected at s=13 TeV with the ATLAS
detector. The data are consistent with the estimated
background and are used to set upper limits on the
production cross section of Higgs-boson pairs times
branching ratio to bbbb for both nonresonant and resonant
production. In the case of resonant production of
Kaluza-Klein gravitons within the Randall-Sundrum model,
upper limits in the 24 to 91 fb range are obtained for
masses between 600 and 3000 GeV, at the 95% confidence
level. The production cross section times branching ratio
for nonresonant Higgs-boson pairs is also constrained to be
less than 1.22 pb, at the 95% confidence
level.},
Doi = {10.1103/PhysRevD.94.052002},
Key = {fds321172}
}
@article{fds308369,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for pair production of massive particles decaying
into three quarks with the ATLAS detector in √s = 7 TeV pp
collisions at the LHC},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {12},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP12(2012)086},
Abstract = {A search is conducted for hadronic three-body decays of a
new massive coloured particle in √s = 7 TeV pp collisions
at the LHC using an integrated luminosity of 4.6 fb-1
collected by the ATLAS detector. Supersymmetric gluino pair
production in the context of a model with R-parity violation
is used as a benchmark scenario. The analysis is divided
into two search channels, each optimised separately for
their sensitivity to high-mass and low-mass gluino
production. The first search channel uses a stringent
selection on the transverse momentum of the six leading jets
and is performed as a counting experiment. The second search
channel focuses on low-mass gluinos produced with a large
boost. Large-radius jets are selected and the invariant mass
of each of the two leading jets is used as a discriminant
between the signal and the background. The results are found
to be consistent with Standard Model expectations and limits
are set on the allowed gluino mass.[Figure not available:
see fulltext.] © 2012 Cern for the benefit of the ATLAS
collaboration.},
Doi = {10.1007/JHEP12(2012)086},
Key = {fds308369}
}
@article{fds365401,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Search for pair production of scalar leptoquarks decaying
into first- or second-generation leptons and top quarks in
proton–proton collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09009-8},
Abstract = {A search for pair production of scalar leptoquarks, each
decaying into either an electron or a muon and a top quark,
is presented. This is the first leptoquark search using
ATLAS data to investigate top-philic cross-generational
couplings that could provide explanations for recently
observed anomalies in B meson decays. This analysis targets
high leptoquark masses which cause the decay products of
each resultant top quark to be contained within a single
high-pT large-radius jet. The full Run 2 dataset is
exploited, consisting of 139fb-1 of data collected from
proton–proton collisions at s=13TeV from 2015 to 2018 with
the ATLAS detector at the CERN Large Hadron Collider. In the
absence of any significant deviation from the background
expectation, lower limits on the leptoquark masses are set
at 1480GeV and 1470GeV for the electron and muon channel,
respectively.},
Doi = {10.1140/epjc/s10052-021-09009-8},
Key = {fds365401}
}
@article{fds308736,
Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Bensinger, J and Beretvas, A and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Bromberg, C and Brozovic, M and Brubaker,
E and Bruner, N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers,
W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, M-T and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, JY and Chung, W-H and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Colijn, AP and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson,
R and Dagenhart, D and D'Auria, S and De Cecco and S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo,
T and Eddy, N and Einsweiler, K and Engels, E and Erbacher, R and Errede,
D and Errede, S and Eusebi, R and Fan, Q and Farrington, S and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher,
B and Flores-Castillo, LR and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Gerstein, E and Giagu, S and Giannetti, P and Giolo, K and Giordani, M and Giromini, P and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Gresele, A and Grim, G and Grosso-Pilcher,
C and Guenther, M and Guillian, G and Guimaraes da Costa and J and Haas,
RM and Haber, C and Hahn, SR and Halkiadakis, E and Hall, C and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss,
A and Hennecke, M and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hollebeek, R and Holloway, L and Hou, S and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Issever, C and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iwai, J and Iwata, Y and Iyutin,
B and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Kang, J and Karagoz Unel and M and Karr, K and Kartal, S and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster,
B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, TH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kotelnikov, K and Kovacs, E and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kurino, K and Kuwabara, T and Kuznetsova, N and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lannon, K and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Le, Y and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Liu, JB and Liu, T and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, NS and Loginov, A and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Manca, G and Mariotti, M and Martignon, G and Martin, M and Martin, A and Martin, V and Martínez, M and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Miyazaki, Y and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Napora, R and Niell, F and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Neuberger, D and Newman-Holmes, C and Ngan, C-YP and Nigmanov, T and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Pescara, L and Phillips, TJ and Piacentino,
G and Piedra, J and Pitts, KT and Pompos, A and Pondrom, L and Pope, G and Pratt, T and Prokoshin, F and Proudfoot, J and Ptohos, F and Pukhov, O and Punzi, G and Rademacker, J and Rakitine, A and Ratnikov, F and Ray, H and Reher, D and Reichold, A and Renton, P and Rescigno, M and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson,
WJ and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Ryan, D and Safonov, A and St Denis and R and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi,
L and Sarkar, S and Sato, H and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
AJ and Sliwa, K and Snider, FD and Snihur, R and Solodsky, A and Spalding,
J and Speer, T and Spezziga, M and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sukhanov, A and Sumorok,
K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, RJ and Teng, PK and Terashi, K and Tether, S and Thom, J and Thompson, AS and Thomson, E and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tonelli, D and Tonnesmann,
M and Toyoda, H and Trischuk, W and De Troconiz and JF and Tseng, J and Tsybychev, D and Turini, N and Ukegawa, F and Unverhau, T and Vaiciulis,
T and Valls, J and Varganov, A and Vataga, E and Vejcik, S and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev,
I},
Title = {Search for pair production of scalar top quarks in R-parity
violating decay modes in pp collisions at square root of
s=1.8 TeV.},
Journal = {Physical review letters},
Volume = {92},
Number = {5},
Pages = {051803},
Year = {2004},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.92.051803},
Abstract = {We present the results of a search for pair production of
scalar top quarks (t(1)) in an R-parity violating
supersymmetry scenario in 106 pb(-1) of pp collisions at
square root of s=1.8 TeV collected by the Collider Detector
at Fermilab. In this mode each t(1) decays into a tau lepton
and a b quark. We search for events with two tau's, one
decaying leptonically (e or mu) and one decaying
hadronically, and two jets. No candidate events pass our
final selection criteria. We set a 95% confidence level
lower limit on the t(1) mass at 122 GeV/c(2) for
Br(t(1)-->tau b)=1.},
Doi = {10.1103/physrevlett.92.051803},
Key = {fds308736}
}
@article{fds308325,
Author = {Aaltonen, T and Albin, E and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson,
JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Search for pair production of strongly interacting particles
decaying to pairs of jets in pp collisions at √s=1.96
TeV.},
Journal = {Physical review letters},
Volume = {111},
Number = {3},
Pages = {031802},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.111.031802},
Abstract = {We present a search for the pair production of a narrow
nonstandard-model strongly interacting particle that decays
to a pair of quarks or gluons, leading to a final state with
four hadronic jets. We consider both nonresonant production
via an intermediate gluon as well as resonant production via
a distinct nonstandard-model intermediate strongly
interacting particle. We use data collected by the CDF
experiment in proton-antiproton collisions at √[s]=1.96
TeV corresponding to an integrated luminosity of 6.6 fb(-1).
We find the data to be consistent with nonresonant
production. We report limits on σ(pp[over ¯]→jjjj) as a
function of the masses of the hypothetical intermediate
particles. Upper limits on the production cross sections for
nonstandard-model particles in several resonant and
nonresonant processes are also derived.},
Doi = {10.1103/physrevlett.111.031802},
Key = {fds308325}
}
@article{fds308476,
Author = {Aaltonen, and T, and others},
Title = {Search for Pair Production of Supersymmetric Top Quarks in
Dilepton Events from $p\bar{p}$ Collisions at $\sqrt{s}$ =
1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {25},
Pages = {251801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.251801},
Abstract = {http://arxiv.org/abs/0912.1308},
Doi = {10.1103/PhysRevLett.104.251801},
Key = {fds308476}
}
@article{fds375897,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez, AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Search for pair production of third-generation leptoquarks
decaying into a bottom quark and a τ -lepton with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {11},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-12104-7},
Abstract = {A search for pair-produced scalar or vector leptoquarks
decaying into a b-quark and a τ -lepton is presented using
the full LHC Run 2 (2015–2018) data sample of 139 fb - 1
collected with the ATLAS detector in proton–proton
collisions at a centre-of-mass energy of s=13 TeV. Events in
which at least one τ -lepton decays hadronically are
considered, and multivariate discriminants are used to
extract the signals. No significant deviations from the
Standard Model expectation are observed and 95%
confidence-level upper limits on the production
cross-section are derived as a function of leptoquark mass
and branching ratio B into a τ -lepton and b-quark. For
scalar leptoquarks, masses below 1460 GeV are excluded
assuming B= 100 %, while for vector leptoquarks the
corresponding limit is 1650 GeV (1910 GeV) in the
minimal-coupling (Yang–Mills) scenario.},
Doi = {10.1140/epjc/s10052-023-12104-7},
Key = {fds375897}
}
@article{fds365397,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler,
A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and An, F and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
Bella, L and Aranzabal, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin, JF and Argyropoulos,
S},
Title = {Search for pair production of third-generation scalar
leptoquarks decaying into a top quark and a τ-lepton in pp
collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {6},
Year = {2021},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2021)179},
Abstract = {A search for pair production of third-generation scalar
leptoquarks decaying into a top quark and a τ-lepton is
presented. The search is based on a dataset of pp collisions
at s = 13 TeV recorded with the ATLAS detector during Run 2
of the Large Hadron Collider, corresponding to an integrated
luminosity of 139 fb−1. Events are selected if they have
one light lepton (electron or muon) and at least one
hadronically decaying τ -lepton, or at least two light
leptons. In addition, two or more jets, at least one of
which must be identified as containing b-hadrons, are
required. Six final states, defined by the multiplicity and
flavour of lepton candidates, are considered in the
analysis. Each of them is split into multiple event
categories to simultaneously search for the signal and
constrain several leading backgrounds. The signal-rich event
categories require at least one hadronically decaying
τ-lepton candidate and exploit the presence of energetic
final-state objects, which is characteristic of signal
events. No significant excess above the Standard Model
expectation is observed in any of the considered event
categories, and 95% CL upper limits are set on the
production cross section as a function of the leptoquark
mass, for different assumptions about the branching
fractions into tτ and bν. Scalar leptoquarks decaying
exclusively into tτ are excluded up to masses of 1.43 TeV
while, for a branching fraction of 50% into tτ, the lower
mass limit is 1.22 TeV. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP06(2021)179},
Key = {fds365397}
}
@article{fds335596,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Search for pair production of up-type vector-like quarks and
for four-top-quark events in final states with multiple
b-jets with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {7},
Publisher = {Springer Nature},
Year = {2018},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2018)089},
Abstract = {A search for pair production of up-type vector-like quarks
(T) with a significant branching ratio into a top quark and
either a Standard Model Higgs boson or a Z boson is
presented. The same analysis is also used to search for
four-top-quark production in several new physics scenarios.
The search is based on a dataset of pp collisions at s=13
TeV recorded in 2015 and 2016 with the ATLAS detector at the
CERN Large Hadron Collider and corresponds to an integrated
luminosity of 36.1 fb-1. Data are analysed in the
lepton+jets final state, characterised by an isolated
electron or muon with high transverse momentum, large
missing transverse momentum and multiple jets, as well as
the jets + ETmiss final state, characterised by multiple
jets and large missing transverse momentum. The search
exploits the high multiplicity of jets identified as
originating from b-quarks, and the presence of boosted,
hadronically decaying top quarks and Higgs bosons
reconstructed as large-radius jets, characteristic of signal
events. No significant excess above the Standard Model
expectation is observed, and 95% CL upper limits are set on
the production cross sections for the different signal
processes considered. These cross-section limits are used to
derive lower limits on the mass of a vector-like T quark
under several branching ratio hypotheses assuming
contributions from T ? W b, Zt, Ht decays. The 95% CL
observed lower limits on the T quark mass range between 0.99
TeV and 1.43 TeV for all possible values of the branching
ratios into the three decay modes considered, significantly
extending the reach beyond that of previous searches.
Additionally, upper limits on anomalous four-top-quark
production are set in the context of an effective field
theory model, as well as in an universal extra dimensions
model.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP07(2018)089},
Key = {fds335596}
}
@article{fds325311,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for pair-produced long-lived neutral particles
decaying to jets in the ATLAS hadronic calorimeter in pp
collisions at s=8TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {743},
Pages = {15-34},
Publisher = {Elsevier BV},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2015.02.015},
Abstract = {The ATLAS detector at the Large Hadron Collider at CERN is
used to search for the decay of a scalar boson to a pair of
long-lived particles, neutral under the Standard Model gauge
group, in 20.3fb-1 of data collected in proton-proton
collisions at s=8TeV. This search is sensitive to long-lived
particles that decay to Standard Model particles producing
jets at the outer edge of the ATLAS electromagnetic
calorimeter or inside the hadronic calorimeter. No
significant excess of events is observed. Limits are
reported on the product of the scalar boson production cross
section times branching ratio into long-lived neutral
particles as a function of the proper lifetime of the
particles. Limits are reported for boson masses from 100 GeV
to 900 GeV, and a long-lived neutral particle mass from 10
GeV to 150 GeV.},
Doi = {10.1016/j.physletb.2015.02.015},
Key = {fds325311}
}
@article{fds321334,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for pair-produced third-generation squarks decaying
via charm quarks or in compressed supersymmetric scenarios
in pp collisions at √s =8TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.90.052008},
Abstract = {Results of a search for supersymmetry via direct production
of third-generation squarks are reported, using 20.3fb-1 of
proton-proton collision data at s=8TeV recorded by the ATLAS
experiment at the LHC in 2012. Two different analysis
strategies based on monojetlike and c-tagged event
selections are carried out to optimize the sensitivity for
direct top squark-pair production in the decay channel to a
charm quark and the lightest neutralino (t∼1→c+χ∼10)
across the top squark-neutralino mass parameter space. No
excess above the Standard Model background expectation is
observed. The results are interpreted in the context of
direct pair production of top squarks and presented in terms
of exclusion limits in the (mt∼1, mχ∼10) parameter
space. A top squark of mass up to about 240 GeV is excluded
at 95% confidence level for arbitrary neutralino masses,
within the kinematic boundaries. Top squark masses up to 270
GeV are excluded for a neutralino mass of 200 GeV. In a
scenario where the top squark and the lightest neutralino
are nearly degenerate in mass, top squark masses up to 260
GeV are excluded. The results from the monojetlike analysis
are also interpreted in terms of compressed scenarios for
top squark-pair production in the decay channel
t∼1→b+ff′+χ∼10 and sbottom pair production with
b∼1→b+χ∼10, leading to a similar exclusion for nearly
mass-degenerate third-generation squarks and the lightest
neutralino. The results in this paper significantly extend
previous results at colliders.},
Doi = {10.1103/PhysRevD.90.052008},
Key = {fds321334}
}
@article{fds375918,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Search for pair-produced vector-like top and bottom partners
in events with large missing transverse momentum in pp
collisions with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {8},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11790-7},
Abstract = {A search for pair-produced vector-like quarks using events
with exactly one lepton (e or μ), at least four jets
including at least one b-tagged jet, and large missing
transverse momentum is presented. Data from proton–proton
collisions at a centre-of-mass energy of s= 13 TeV ,
recorded by the ATLAS detector at the LHC from 2015 to 2018
and corresponding to an integrated luminosity of 139 fb - 1
, are analysed. Vector-like partners T and B of the top and
bottom quarks are considered, as is a vector-like X with
charge + 5 / 3 , assuming their decay into a W, Z, or Higgs
boson and a third-generation quark. No significant
deviations from the Standard Model expectation are observed.
Upper limits on the production cross-section of T and B
quark pairs as a function of their mass are derived for
various decay branching ratio scenarios. The strongest lower
limits on the masses are 1.59 TeV assuming mass-degenerate
vector-like quarks and branching ratios corresponding to the
weak-isospin doublet model, and 1.47 TeV (1.46 TeV) for
exclusive T→ Zt (B/ X→ Wt) decays. In addition, lower
limits on the T and B quark masses are derived for all
possible branching ratios.},
Doi = {10.1140/epjc/s10052-023-11790-7},
Key = {fds375918}
}
@article{fds375917,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Search for pair-production of vector-like quarks in pp
collision events at s=13 TeV with at least one leptonically
decaying Z boson and a third-generation quark with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138019},
Abstract = {A search for the pair-production of vector-like quarks
optimized for decays into a Z boson and a third-generation
Standard Model quark is presented, using the full Run 2
dataset corresponding to 139fb−1 of pp collisions at
s=13TeV, collected in 2015–2018 with the ATLAS detector at
the Large Hadron Collider. The targeted final state is
characterized by the presence of a Z boson with high
transverse momentum, reconstructed from a pair of
same-flavour leptons with opposite-sign charges, as well as
by the presence of b-tagged jets and high-transverse-momentum
large-radius jets reconstructed from calibrated
smaller-radius jets. Events with exactly two or at least
three leptons are used, which are further categorized by the
presence of boosted W, Z, and Higgs bosons and top quarks.
The categorization is performed using a neural-network-based
boosted object tagger to enhance the sensitivity to signal
relative to the background. No significant excess above the
background expectation is observed and exclusion limits at
95% confidence level are set on the masses of the
vector-like partners T and B of the top and bottom quarks,
respectively. The limits depend on the branching ratio
configurations and, in the case of 100% branching ratio for
T→Zt and 100% branching ratio for B→Zb, this search sets
the most stringent limits to date, allowing mT>1.60TeV and
mB>1.42TeV, respectively.},
Doi = {10.1016/j.physletb.2023.138019},
Key = {fds375917}
}
@article{fds375891,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Search for pairs of muons with small displacements in pp
collisions at s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {846},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138172},
Abstract = {A search for new phenomena giving rise to pairs of opposite
electrically charged muons with impact parameters in the
millimeter range is presented, using 139 fb−1 of s=13 TeV
pp collision data from the ATLAS detector at the LHC. The
search targets the gap in coverage between existing searches
targeting final states with leptons with large displacement
and prompt leptons. No significant excess over the
background expectation is observed and exclusion limits are
set on the mass of long-lived scalar supersymmetric
muon-partners (smuons) with much lower lifetimes than
previously targeted by displaced muon searches. Smuon
lifetimes down to 1 ps are excluded for a smuon mass of 100
GeV, and smuon masses up to 520 GeV are excluded for a
proper lifetime of 10 ps, at 95% confidence level. Finally,
model-independent limits are set on the contribution from
new phenomena to the signal-region yields.},
Doi = {10.1016/j.physletb.2023.138172},
Key = {fds375891}
}
@article{fds365428,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Search for pairs of scalar leptoquarks decaying into quarks
and electrons or muons in √s = 13 TeV pp collisions with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2020)112},
Abstract = {A search for new-physics resonances decaying into a lepton
and a jet performed by the ATLAS experiment is presented.
Scalar leptoquarks pair-produced in pp collisions at s = 13
TeV at the Large Hadron Collider are considered using an
integrated luminosity of 139 fb−1, corresponding to the
full Run 2 dataset. They are searched for in events with two
electrons or two muons and two or more jets, including jets
identified as arising from the fragmentation of c- or
b-quarks. The observed yield in each channel is consistent
with the Standard Model background expectation. Leptoquarks
with masses below 1.8 TeV and 1.7 TeV are excluded in the
electron and muon channels, respectively, assuming a
branching ratio into a charged lepton and a quark of 100%,
with minimal dependence on the quark flavour. Upper limits
on the aforementioned branching ratio are also given as a
function of the leptoquark mass. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP10(2020)112},
Key = {fds365428}
}
@article{fds365416,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Search for phenomena beyond the Standard Model in events
with large b-jet multiplicity using the ATLAS detector at
the LHC},
Journal = {European Physical Journal C},
Volume = {81},
Number = {1},
Year = {2021},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08730-0},
Abstract = {A search is presented for new phenomena in events
characterised by high jet multiplicity, no leptons
(electrons or muons), and four or more jets originating from
the fragmentation of b-quarks (b-jets). The search uses
139fb-1 of s = 13 TeV proton–proton collision data
collected by the ATLAS experiment at the Large Hadron
Collider during Run 2. The dominant Standard Model
background originates from multijet production and is
estimated using a data-driven technique based on an
extrapolation from events with low b-jet multiplicity to the
high b-jet multiplicities used in the search. No significant
excess over the Standard Model expectation is observed and
95% confidence-level limits that constrain simplified models
of R-parity-violating supersymmetry are determined. The
exclusion limits reach 950 GeV in top-squark mass in the
models considered.},
Doi = {10.1140/epjc/s10052-020-08730-0},
Key = {fds365416}
}
@article{fds321219,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for photonic signatures of gauge-mediated
supersymmetry in 8 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.92.072001},
Abstract = {A search is presented for photonic signatures motivated by
generalized models of gauge-mediated supersymmetry breaking.
This search makes use of 20.3 fb-1 of proton-proton
collision data at √s = 8 TeV recorded by the ATLAS
detector at the LHC, and explores models dominated by both
strong and electroweak production of supersymmetric partner
states. Four experimental signatures incorporating an
isolated photon and significant missing transverse momentum
are explored. These signatures include events with an
additional photon, lepton, b-quark jet, or jet activity not
associated with any specific underlying quark flavor. No
significant excess of events is observed above the Standard
Model prediction and model-dependent 95% confidence-level
exclusion limits are set.},
Doi = {10.1103/PhysRevD.92.072001},
Key = {fds321219}
}
@article{fds321265,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Search for production of an Υ (1 S) meson in association
with a W or Z boson using the full 1.96 TeV pp ¯ collision
data set at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.91.052011},
Abstract = {Production of the Υ(1S) meson in association with a vector
boson is a rare process in the standard model with a cross
section predicted to be below the sensitivity of the
Tevatron. Observation of this process could signify
contributions not described by the standard model or reveal
limitations with the current nonrelativistic
quantum-chromodynamic models used to calculate the cross
section. We perform a search for this process using the full
Run II data set collected by the CDF II detector
corresponding to an integrated luminosity of 9.4fb-1. The
search considers the Υ→μμ decay and the decay of the W
and Z bosons into muons and electrons. In these purely
leptonic decay channels, we observe one ΥW candidate with
an expected background of 1.2±0.5 events, and one ΥZ
candidate with an expected background of 0.1±0.1 events.
Both observations are consistent with the predicted
background contributions. The resulting upper limits on the
cross section for Υ+W/Z production are the most sensitive
reported from a single experiment and place restrictions on
potential contributions from non-standard-model
physics.},
Doi = {10.1103/PhysRevD.91.052011},
Key = {fds321265}
}
@article{fds308437,
Author = {Aaltonen, and T, and al, E},
Title = {Search for Production of Heavy Particles Decaying to Top
Quarks and Invisible Particles in $p\overline{p}$ Collisions
at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {19},
Pages = {191801},
Publisher = {American Physical Society},
Year = {2011},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.191801},
Abstract = {We present a search for a new particle T' decaying to top
quark via T' → t + X, where X is an invisible particle. In
a data sample with 4.8 fb(-1) of integrated luminosity
collected by the CDF II detector at Fermilab in pp
collisions with √s = 1.96 TeV, we search for pair
production of T' in the lepton + jets channel, pp → tt + X
+ X → ℓνbqq'b + X + X. We interpret our results
primarily in terms of a model where T' are exotic fourth
generation quarks and X are dark matter particles. Current
direct and indirect bounds on such exotic quarks restrict
their masses to be between 300 and 600 GeV/c2, the dark
matter particle mass being anywhere below m(T'). The data
are consistent with standard model expectations, and we set
95% confidence level limits on the generic production of
T'T' → tt + X + X. For the dark matter model we exclude T'
at 95% confidence level up to m(T') = 360 GeV/c2 for
m(X) ≤ 100 GeV/c2.},
Doi = {10.1103/PhysRevLett.106.191801},
Key = {fds308437}
}
@article{fds321234,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for production of vector-like quark pairs and of four
top quarks in the lepton-plus-jets final state in pp
collisions at √s = 8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {8},
Publisher = {Springer Nature},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2015)105},
Abstract = {A search for pair production of vector-like quarks, both
up-type (T) and down-type (B), as well as for four-top-quark
production, is presented. The search is based on pp
collisions at (Formula presented.) TeV recorded in 2012 with
the ATLAS detector at the CERN Large Hadron Collider and
corresponding to an integrated luminosity of 20.3 fb−1.
Data are analysed in the lepton-plus-jets final state,
characterised by an isolated electron or muon with high
transverse momentum, large missing transverse momentum and
multiple jets. Dedicated analyses are performed targeting
three cases: a T quark with significant branching ratio to a
W boson and a b-quark (TT¯→Wb+X), and both a T quark and
a B quark with significant branching ratio to a Higgs boson
and a third-generation quark (TT¯→Ht+XandBB¯→Hb+X
respectively). No significant excess of events above the
Standard Model expectation is observed, and 95% CL lower
limits are derived on the masses of the vector-like T and B
quarks under several branching ratio hypotheses assuming
contributions from T → Wb, Zt, Ht and B → Wt, Zb, Hb
decays. The 95% CL observed lower limits on the T quark mass
range between 715 GeV and 950 GeV for all possible values of
the branching ratios into the three decay modes, and are the
most stringent constraints to date. Additionally, the most
restrictive upper bounds on four-top-quark production are
set in a number of new physics scenarios.},
Doi = {10.1007/JHEP08(2015)105},
Key = {fds321234}
}
@article{fds321289,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca,
D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Search for production of [Formula: see text] resonances
decaying to a lepton, neutrino and jets in [Formula: see
text] collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {5},
Pages = {209},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3425-6},
Abstract = {A search is presented for narrow diboson resonances decaying
to [Formula: see text] or [Formula: see text] in the final
state where one [Formula: see text] boson decays
leptonically (to an electron or a muon plus a neutrino) and
the other [Formula: see text] boson decays hadronically. The
analysis is performed using an integrated luminosity of
20.3 fb[Formula: see text] of [Formula: see text]
collisions at [Formula: see text] TeV collected by the
ATLAS detector at the large hadron collider. No evidence for
resonant diboson production is observed, and resonance
masses below 700 and 1490 GeV are excluded at 95 %
confidence level for the spin-2 Randall-Sundrum bulk
graviton [Formula: see text] with coupling constant of 1.0
and the extended gauge model [Formula: see text] boson
respectively.},
Doi = {10.1140/epjc/s10052-015-3425-6},
Key = {fds321289}
}
@article{fds308282,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canelli, F and Canepa,
A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin,
V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba,
J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
Title = {Search for quantum black hole production in
high-invariant-mass lepton+jet final states using pp
collisions at √s=8 TeV and the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {112},
Number = {9},
Pages = {091804},
Year = {2014},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.112.091804},
Abstract = {This Letter presents a search for quantum black-hole
production using 20.3 fb-1 of data collected with the ATLAS
detector in pp collisions at the LHC at √s = 8 TeV. The
quantum black holes are assumed to decay into a final state
characterized by a lepton (electron or muon) and a jet. In
either channel, no event with a lepton-jet invariant mass of
3.5 TeV or more is observed, consistent with the expected
background. Limits are set on the product of cross sections
and branching fractions for the lepton+jet final states of
quantum black holes produced in a search region for
invariant masses above 1 TeV. The combined 95% confidence
level upper limit on this product for quantum black holes
with threshold mass above 3.5 TeV is 0.18 fb. This limit
constrains the threshold quantum black-hole mass to be above
5.3 TeV in the model considered.},
Doi = {10.1103/physrevlett.112.091804},
Key = {fds308282}
}
@article{fds376313,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V},
Title = {Search for quantum black hole production in lepton + jet
final states using proton-proton collisions at vs = 13 TeV
with the ATLAS detector},
Journal = {Physical Review D},
Volume = {109},
Number = {3},
Year = {2024},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.109.032010},
Abstract = {A search for quantum black holes in electron + jet and muon
+ jet invariant mass spectra is performed with 140 fb-1 of
data collected by the ATLAS detector in proton-proton
collisions at √s = 13 TeV at the Large Hadron Collider.
The observed invariant mass spectrum of lepton + jet pairs
is consistent with Standard Model expectations. Upper limits
are set at 95% confidence level on the production cross
section times branching fractions for quantum black holes
decaying into a lepton and a quark in a search region with
invariant mass above 2.0 TeV. The resulting quantum black
hole lower mass threshold limit is 9.2 TeV in the
Arkani-Hamed-Dimopoulos-Dvali model, and 6.8 TeV in the
Randall-Sundrum model.},
Doi = {10.1103/PhysRevD.109.032010},
Key = {fds376313}
}
@article{fds308786,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson,
R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin,
T and Dittmann, JR and Dominguez, A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erbacher, R and Errede, D and Errede, S and Fan, Q and Feild,
RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman,
J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov, I and Goshaw,
AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kotwal, AV and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis,
JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima,
K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto,
WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt,
M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel,
S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding,
J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda,
H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
F and Vaiciulis, T and Valls, J and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters,
D and Watts, T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Search for quark-lepton compositeness and a heavy W′ Boson
using the eν channel in pp̄ Collisions at √s = 1.8
TeV},
Journal = {Physical Review Letters},
Volume = {87},
Number = {23},
Pages = {2318031-2318036},
Year = {2001},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.87.231803},
Abstract = {A study on searches for quark-lepton compositeness and a
heavy boson at high electron-neutrino transverse mass was
presented. The data collected in pp̄ collisions at √s=1.8
TeV was used for the analysis. The data obtained is found to
be consistent with the standard model (SM)
predictions.},
Doi = {10.1103/physrevlett.87.231803},
Key = {fds308786}
}
@article{fds365371,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling,
JH},
Title = {Search for R-parity-violating supersymmetry in a final state
containing leptons and many jets with the ATLAS experiment
using √s=13TeV proton–proton collision
data},
Journal = {European Physical Journal C},
Volume = {81},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09761-x},
Abstract = {A search for R-parity-violating supersymmetry in final
states characterized by high jet multiplicity, at least one
isolated light lepton and either zero or at least three
b-tagged jets is presented. The search uses 139fb-1 of
s=13TeV proton–proton collision data collected by the
ATLAS experiment during Run 2 of the Large Hadron Collider.
The results are interpreted in the context of
R-parity-violating supersymmetry models that feature gluino
production, top-squark production, or electroweakino
production. The dominant sources of background are estimated
using a data-driven model, based on observables at medium
jet multiplicity, to predict the b-tagged jet multiplicity
distribution at the higher jet multiplicities used in the
search. Machine-learning techniques are used to reach
sensitivity to electroweakino production, extending the
data-driven background estimation to the shape of the
machine-learning discriminant. No significant excess over
the Standard Model expectation is observed and exclusion
limits at the 95% confidence level are extracted, reaching
as high as 2.4 TeV in gluino mass, 1.35 TeV in top-squark
mass, and 320 (365) GeV in higgsino (wino)
mass.},
Doi = {10.1140/epjc/s10052-021-09761-x},
Key = {fds365371}
}
@article{fds308370,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for R-parity-violating supersymmetry in events with
four or more leptons in √s =7 TeV pp collisions with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {12},
Publisher = {Springer Nature},
Year = {2012},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2012)124},
Abstract = {A search for new phenomena in final states with four or more
leptons (electrons or muons) is presented. The analysis is
based on 4.7 fb-1 of √s =7 TeV proton-proton collisions
delivered by the Large Hadron Collider and recorded with the
ATLAS detector. Observations are consistent with Standard
Model expectations in two signal regions: one that requires
moderate values of missing transverse momentum and another
that requires large effective mass. The results are
interpreted in a simplified model of R-parity-violating
supersymmetry in which a 95% CL exclusion region is set for
charged wino masses up to 540 GeV. In an R-parity-violating
MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are
excluded for 10 < tan β < 40. © 2012 Cern for the benefit
of the ATLAS collaboration.},
Doi = {10.1007/JHEP12(2012)124},
Key = {fds308370}
}
@article{fds331632,
Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Bensinger, J and Beretvas, A and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and Bromberg, C and Brozovic, M and Brubaker, E and Bruner,
N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, M and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, JY and Chung, W and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Colijn, AP and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R and Dagenhart, D and D’Auria, S},
Title = {Search for radiative [Formula Presented]-hadron decays in
[Formula Presented] collisions at [Formula
Presented]},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {66},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.66.112002},
Abstract = {We have performed a search for radiative b-hadron decays
using events produced in [Formula Presented] collisions at
[Formula Presented] and collected by the Collider Detector
at Fermilab. The decays we considered were [Formula
Presented] [Formula Presented] [Formula Presented] and their
charge conjugates. Two independent methods to identify
photons from such decays were employed. In the first method,
the photon was detected in the electromagnetic calorimeter.
In the second method, the photon was identified by an
electron-positron pair produced through the external photon
conversion before the tracking detector volume. By combining
the two methods we obtain upper limits on the branching
fractions for the [Formula Presented] [Formula Presented]
and [Formula Presented] radiative decays which, at the 95%
confidence level, are found to be [Formula Presented]
[Formula Presented] and [Formula Presented] © 2002 The
American Physical Society.},
Doi = {10.1103/PhysRevD.66.112002},
Key = {fds331632}
}
@article{fds308359,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for resonances decaying into top-quark pairs using
fully hadronic decays in pp collisions with ATLAS at √s=7
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {1},
Publisher = {Springer Nature},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP01(2013)116},
Abstract = {A search for resonances produced in 7 TeV proton-proton
collisions and decaying into top-quark pairs is described.
In this Letter events where the top-quark decay produces two
massive jets with large transverse momenta recorded with the
ATLAS detector at the Large Hadron Collider are considered.
Two techniques that rely on jet substructure are used to
separate top-quark jets from those arising from light quarks
and gluons. In addition, each massive jet is required to
have evidence of an associated bottom-quark decay. The data
are consistent with the Standard Model, and limits can be
set on the production cross section times branching fraction
of a Z′ boson and a Kaluza-Klein gluon resonance. These
limits exclude, at the 95% credibility level, Z′ bosons
with masses 0.70-1.00 TeV as well as 1.28-1.32 TeV and
Kaluza-Klein gluons with masses 0.70-1.62 TeV. © 2013 Cern
for the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP01(2013)116},
Key = {fds308359}
}
@article{fds321229,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Anzà, F and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bianchi, L and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino,
P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon,
CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat,
P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano,
I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino,
G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos,
F and Punzi, G and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Search for Resonances Decaying to Top and Bottom Quarks with
the CDF Experiment.},
Journal = {Physical review letters},
Volume = {115},
Number = {6},
Pages = {061801},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.115.061801},
Abstract = {We report on a search for charged massive resonances
decaying to top (t) and bottom (b) quarks in the full data
set of proton-antiproton collisions at a center-of-mass
energy of √[s]=1.96 TeV collected by the CDF II
detector at the Tevatron, corresponding to an integrated
luminosity of 9.5 fb(-1). No significant excess above
the standard model background prediction is observed. We set
95% Bayesian credibility mass-dependent upper limits on the
heavy charged-particle production cross section times
branching ratio to tb. Using a standard model extension with
a W'→tb and left-right-symmetric couplings as a benchmark
model, we constrain the W' mass and couplings in the
300-900 GeV/c(2) range. The limits presented here are
the most stringent for a charged resonance with mass in the
range 300-600 GeV/c(2) decaying to top and bottom
quarks.},
Doi = {10.1103/physrevlett.115.061801},
Key = {fds321229}
}
@article{fds321163,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Search for resonances in diphoton events at √s=13 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {9},
Publisher = {Springer Nature},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2016)001},
Abstract = {Searches for new resonances decaying into two photons in the
ATLAS experiment at the CERN Large Hadron Collider are
described. The analysis is based on proton-proton collision
data corresponding to an integrated luminosity of 3.2 fb−1
at s=13 TeV recorded in 2015. Two searches are performed,
one targeted at a spin-2 particle of mass larger than 500
GeV, using Randall-Sundrum graviton states as a benchmark
model, and one optimized for a spin-0 particle of mass
larger than 200 GeV. Varying both the mass and the decay
width, the most significant deviation from the
background-only hypothesis is observed at a diphoton
invariant mass around 750 GeV with local significances of
3.8 and 3.9 standard deviations in the searches optimized
for a spin-2 and spin-0 particle, respectively. The global
significances are estimated to be 2.1 standard deviations
for both analyses. The consistency between the data
collected at 13 TeV and 8 TeV is also evaluated. Limits on
the production cross section times branching ratio to two
photons for the two resonance types are reported.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP09(2016)001},
Key = {fds321163}
}
@article{fds321206,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for resonances in the mass distribution of jet pairs
with one or two jets identified as b-jets in proton–proton
collisions at s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {759},
Pages = {229-246},
Publisher = {Elsevier BV},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2016.05.064},
Abstract = {Searches for high-mass resonances in the dijet invariant
mass spectrum with one or two jets identified as b-jets are
performed using an integrated luminosity of 3.2 fb−1 of
proton–proton collisions with a centre-of-mass energy of
s=13 TeV recorded by the ATLAS detector at the Large Hadron
Collider. No evidence of anomalous phenomena is observed in
the data, which are used to exclude, at 95% credibility
level, excited b⁎ quarks with masses from 1.1 TeV to 2.1
TeV and leptophobic Z′ bosons with masses from 1.1 TeV to
1.5 TeV. Contributions of a Gaussian signal shape with
effective cross sections ranging from approximately 0.4 to
0.001 pb are also excluded in the mass range 1.5–5.0
TeV.},
Doi = {10.1016/j.physletb.2016.05.064},
Key = {fds321206}
}
@article{fds308447,
Author = {Aaltonen, TEA},
Title = {Search for resonant production of $t\overline{t}$ decaying
to jets in $p\overline{p}$ collisions at
$\sqrt{s}\mathbf{=}1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society},
Year = {2011},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.84.072003},
Abstract = {This paper reports a search for nonstandard model topquark
resonances, Z′, decaying to tt̄→W+bW -b̄, where both W
decay to quarks. We examine the top-antitop quark invariant
mass spectrum for the presence of narrow resonant states.
The search uses a data sample of pp̄ collisions at a center
of mass energy of 1.96 TeV collected by the CDF II detector
at the Fermilab Tevatron, with an integrated luminosity of
2.8fb-1. No evidence for top-antitop quark resonant
production is found. We place upper limits on the production
cross section times branching ratio for a specific topcolor
assisted technicolor model in which the Z′ has a width of
Γ Z′=0.012MZ′. Within this model, we exclude a Z′
boson with masses below 805GeV/c2 at the 95% confidence
level. © 2011 American Physical Society.},
Doi = {10.1103/PhysRevD.84.072003},
Key = {fds308447}
}
@article{fds308448,
Author = {Aaltonen, TEA},
Title = {Search for resonant production of $t\overline{t}$ pairs in
$4.8{\,}{\,}{\mathrm{fb}}^{\mathbf{-}1}$ of integrated
luminosity of $p\overline{p}$ collisions at
$\sqrt{s}\mathbf{=}1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {7},
Pages = {072004},
Publisher = {American Physical Society},
Year = {2011},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.84.072004},
Abstract = {We search for resonant production of tt̄ pairs in 4.8fb-1
integrated luminosity of pp̄ collision data at √s=1.96TeV
in the lepton+jets decay channel, where one top quark decays
leptonically and the other hadronically. A matrix-element
reconstruction technique is used; for each event a
probability density function of the tt̄ candidate invariant
mass is sampled. These probability density functions are
used to construct a likelihood function, whereby the cross
section for resonant tt̄ production is estimated, given a
hypothetical resonance mass and width. The data indicate no
evidence of resonant production of tt̄ pairs. A benchmark
model of leptophobic Z′→tt̄ is excluded with m
Z′<900GeV/c2 at 95% confidence level. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevD.84.072004},
Key = {fds308448}
}
@article{fds308337,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson,
JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Search for resonant top-antitop production in the lepton
plus jets decay mode using the full CDF data
set.},
Journal = {Physical review letters},
Volume = {110},
Number = {12},
Pages = {121802},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.110.121802},
Abstract = {This Letter reports a search for a narrow resonant state
decaying into two W bosons and two b quarks where one W
boson decays leptonically and the other decays into a
quark-antiquark pair. The search is particularly sensitive
to top-antitop resonant production. We use the full data
sample of proton-antiproton collisions at a center-of-mass
energy of 1.96 TeV collected by the CDF II detector at the
Fermilab Tevatron, corresponding to an integrated luminosity
of 9.45 fb(-1). No evidence for resonant production is
found, and upper limits on the production cross section
times branching ratio for a narrow resonant state are
extracted. Within a specific benchmark model, we exclude a
Z' boson with mass, M(Z'), below 915 GeV/c(2) decaying into
a top-antitop pair at the 95% credibility level assuming a
Z' boson decay width of Γ(Z') = 0.012 M(Z'). This is the
most sensitive search for a narrow qq-initiated tt resonance
in the mass region below 750 GeV/c(2).},
Doi = {10.1103/physrevlett.110.121802},
Key = {fds308337}
}
@article{fds375935,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Search for resonant WZ production in the fully leptonic
final state in proton–proton collisions at √s=13 TeV
with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11437-7},
Abstract = {A search for a WZ resonance, in the fully leptonic final
state (electrons or muons), is performed using 139 fb - 1
of data collected at a centre-of-mass energy of 13 TeV by
the ATLAS detector at the Large Hadron Collider. The results
are interpreted in terms of a singly charged Higgs boson of
the Georgi–Machacek model, produced by WZ fusion, and of a
Heavy Vector Triplet, with the resonance produced by WZ
fusion or the Drell–Yan process. No significant excess
over the Standard Model prediction is observed and limits
are set on the production cross-section times branching
ratio as a function of the resonance mass for these
processes.},
Doi = {10.1140/epjc/s10052-023-11437-7},
Key = {fds375935}
}
@article{fds321274,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
Title = {Search for s-channel single top-quark production in
proton-proton collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {740},
Pages = {118-136},
Publisher = {Elsevier BV},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2014.11.042},
Abstract = {This Letter presents a search at the LHC for s-channel
single top-quark production in proton-proton collisions at a
centre-of-mass energy of 8 TeV. The analyzed data set was
recorded by the ATLAS detector and corresponds to an
integrated luminosity of 20.3 fb-1. Selected events contain
one charged lepton, large missing transverse momentum and
exactly two b-tagged jets. A multivariate event classifier
based on boosted decision trees is developed to discriminate
s-channel single top-quark events from the main background
contributions. The signal extraction is based on a binned
maximum-likelihood fit of the output classifier
distribution. The analysis leads to an upper limit on the
s-channel single top-quark production cross-section of 14.6
pb at the 95% confidence level. The fit gives a
cross-section of σs = 5.0 ± 4.3 pb, consistent with the
Standard Model expectation.},
Doi = {10.1016/j.physletb.2014.11.042},
Key = {fds321274}
}
@article{fds308269,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Vázquez, F and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Search for s-channel single-top-quark production in events
with missing energy plus jets in pp collisions at sqrt[s] =
1.96 TeV.},
Journal = {Physical review letters},
Volume = {112},
Number = {23},
Pages = {231805},
Year = {2014},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.112.231805},
Abstract = {The first search for single-top-quark production from the
exchange of an s-channel virtual W boson using events with
an imbalance in the total transverse energy, b-tagged jets,
and no identified leptons is presented. Assuming the
electroweak production of top quarks of mass 172.5 GeV/c(2)
in the s channel, a cross section of 1.12(-0.57)(+0.61)
(stat+syst) pb with a significance of 1.9 standard
deviations is measured. This measurement is combined with
the result obtained from events with an imbalance in total
transverse momentum, b-tagged jets, and exactly one
identified lepton, yielding a cross section of
1.36(-0.32)(+0.37) (stat+syst) pb, with a significance of
4.2 standard deviations.},
Doi = {10.1103/physrevlett.112.231805},
Key = {fds308269}
}
@article{fds321255,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
Title = {Search for Scalar Charm Quark Pair Production in pp
Collisions at sqrt[s]=8 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {16},
Pages = {161801},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.114.161801},
Abstract = {The results of a dedicated search for pair production of
scalar partners of charm quarks are reported. The search is
based on an integrated luminosity of 20.3 fb^{-1} of pp
collisions at sqrt[s]=8 TeV recorded with the ATLAS
detector at the LHC. The search is performed using events
with large missing transverse momentum and at least two
jets, where the two leading jets are each tagged as
originating from c quarks. Events containing isolated
electrons or muons are vetoed. In an R-parity-conserving
minimal supersymmetric scenario in which a single
scalar-charm state is kinematically accessible, and where it
decays exclusively into a charm quark and a neutralino, 95%
confidence-level upper limits are obtained in the
scalar-charm-neutralino mass plane such that, for neutralino
masses below 200 GeV, scalar-charm masses up to 490 GeV
are excluded.},
Doi = {10.1103/physrevlett.114.161801},
Key = {fds321255}
}
@article{fds321321,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Akesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
Title = {Search for scalar diphoton resonances in the mass range
65-600 GeV with the ATLAS detector in pp collision data at
√s=8 TeV.},
Journal = {Physical review letters},
Volume = {113},
Number = {17},
Pages = {171801},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.113.171801},
Abstract = {A search for scalar particles decaying via narrow resonances
into two photons in the mass range 65-600 GeV is performed
using 20.3 fb(-1) of √s 8 TeV pp collision data
collected with the ATLAS detector at the Large Hadron
Collider. The recently discovered Higgs boson is treated as
a background. No significant evidence for an additional
signal is observed. The results are presented as limits at
the 95% confidence level on the production cross section of
a scalar boson times branching ratio into two photons, in a
fiducial volume where the reconstruction efficiency is
approximately independent of the event topology. The upper
limits set extend over a considerably wider mass range than
previous searches.},
Doi = {10.1103/physrevlett.113.171801},
Key = {fds321321}
}
@article{fds308721,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri,
A and Cerrito, L and Chapman, J and Chen, YC and Chertok, M and Chiarelli,
G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chuang, S and Chung, K and Chung, WH and Chung, YS and Cijliak, M and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway,
J},
Title = {Search for scalar leptoquark pairs decaying to νν̄qq̄ in
pp̄ collisions at s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {11},
Pages = {1-7},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.71.112001},
Abstract = {We report on a search for the pair production of scalar
leptoquarks (LQ), using 191pb-1 of proton-antiproton
collision data recorded by the CDF experiment during Run II
of the Tevatron. The leptoquarks are sought via their decay
into a neutrino and quark yielding missing transverse energy
and several jets of large transverse energy. No evidence for
LQ production is observed, and limits are set on
σ(pp̄→LQLQ̄X→νν̄qq̄X). Using a next-to-leading
order theoretical prediction of the cross section for LQ
production, we exclude first-generation LQ in the mass
interval 78 to 117GeV/c2 at the 95% confidence level for
BR(LQ→νq)=100%. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevD.71.112001},
Key = {fds308721}
}
@article{fds321162,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for scalar leptoquarks in pp collisions at √S =
13TeV with the ATLAS experiment},
Journal = {New Journal of Physics},
Volume = {18},
Number = {9},
Pages = {1-25},
Publisher = {IOP Publishing},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1088/1367-2630/18/9/093016},
Abstract = {An inclusive search for a new-physics signature of
lepton-jet resonances has been performed by the ATLAS
experiment. Scalar leptoquarks, pair-produced in pp
collisions at s √S13 TeV at the large hadron collider,
have been considered. An integrated luminosity of 3.2
fb−1, corresponding to the full 2015 dataset was used.
First (second) generation leptoquarks were sought in events
with two electrons (muons) and two or more jets. The
observed event yield in each channel is consistent with
Standard Model background expectations. The observed
(expected) lower limits on the leptoquark mass at 95%
confidence level are 1100 and 1050 GeV (1160 and 1040 GeV)
for first and second generation leptoquarks, respectively,
assuming a branching ratio into a charged lepton and a quark
of 100%. Upper limits on the aforementioned branching ratio
are also given as a function of leptoquark mass. Compared
with the results of earlier ATLAS searches, the sensitivity
is increased for leptoquark masses above 860 GeV, and the
observed exclusion limits confirm and extend the published
results.},
Doi = {10.1088/1367-2630/18/9/093016},
Key = {fds321162}
}
@article{fds321370,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d’Ascenzo, N and Datta, M and de
Barbaro, P and Dell’Orso, M and Demortier, L and Deninno, M and Devoto, F and d’Errico, M},
Title = {Search for scalar top quark production in (Formula
presented.) collisions at (Formula presented.) = 1.96
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {10},
Publisher = {Springer Nature},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2012)158},
Abstract = {We report on a search for the supersymmetric partner of the
top quark (scalar top) decaying into a charm quark and a
neutralino in (Formula presented.) collisions at (Formula
presented.) = 1.96TeV. The data sample, collected by the CDF
II detector at the Fermilab Tevatron, corresponds to an
integrated luminosity of 2.6 fb<sup>−1</sup>. Candidate
events are selected by requiring two or more jets and a
large imbalance in the transverse momentum. To enhance the
analysis sensitivity, at least one of the jets is required
to be identified as originating from a charm quark using an
algorithm specifically designed for this analysis. The
selected events are in good agreement with standard model
predictions. In the case of large mass splitting between the
scalar top quark and the neutralino we exclude a scalar top
quark mass below 180 GeV/c<sup>2</sup> at 95% confidence
level.},
Doi = {10.1007/JHEP10(2012)158},
Key = {fds321370}
}
@article{fds308716,
Author = {Abulencia, and A, and others},
Title = {Search for second-generation scalar leptoquarks in
$p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {5},
Pages = {051102},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.72.051107},
Abstract = {Results on a search for pair production of second generation
scalar leptoquark in p anti-p collisions at s**(1/2) = 1.96
TeV are reported. The data analyzed were collected by the
CDF detector during the 2002-2003 Tevatron Run II and
correspond to an integrated luminosity of 198 pb-1.
Leptoquarks (LQ) are sought through their decay into
(charged) leptons and quarks, with final state signatures
represented by two muons and jets and one muon, large
transverse missing energy and jets. We observe no evidence
for LQ production and derive 95% C.L. upper limits on the LQ
production cross sections as well as lower limits on their
mass as a function of Beta, where Beta is the branching
fraction for LQ --> mu q.},
Doi = {10.1103/PhysRevD.72.051107},
Key = {fds308716}
}
@article{fds315958,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O},
Title = {Search for single production of a vector-like quark via a
heavy gluon in the 4b final state with the ATLAS detector in
pp collisions at s=8 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {758},
Pages = {249-268},
Publisher = {Elsevier BV},
Year = {2016},
Month = {July},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2016.04.061},
Abstract = {A search is performed for the process pp→G*→BHb-/B-Hb→Hbb-→bb-bb-,
predicted in composite Higgs scenarios, where G* is a heavy
colour octet vector resonance and BH a vector-like quark of
charge -1/3. The data were obtained from pp collisions at a
centre-of-mass energy of 8 TeV corresponding to an
integrated luminosity of 19.5 fb-1, recorded by the ATLAS
detector at the LHC. The largest background, multijet
production, is estimated using a data-driven method. No
significant excess of events with respect to Standard Model
predictions is observed, and upper limits on the production
cross section times branching ratio are set. Comparisons to
the predictions from a specific benchmark model are made,
resulting in lower mass limits in the two-dimensional mass
plane of mG* vs. mBH.},
Doi = {10.1016/j.physletb.2016.04.061},
Key = {fds315958}
}
@article{fds321177,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
LB and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov,
VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella,
G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford,
L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and de
Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich,
LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
DG and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella,
G},
Title = {Search for single production of vector-like quarks decaying
into Wb in pp collisions at [Formula: see
text] TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {8},
Pages = {442},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4281-8},
Abstract = {A search for singly produced vector-like <i>Q</i> quarks,
where <i>Q</i> can be either a <i>T</i> quark with charge
[Formula: see text] or a <i>Y</i> quark with charge
[Formula: see text], is performed in proton-proton
collisions recorded with the ATLAS detector at the LHC. The
dataset corresponds to an integrated luminosity of 20.3
fb[Formula: see text] and was produced with a centre-of-mass
energy of [Formula: see text] TeV. This analysis targets
[Formula: see text] decays where the <i>W</i> boson decays
leptonically. A veto on massive large-radius jets is used to
reject the dominant [Formula: see text] background. The
reconstructed <i>Q</i>-candidate mass, ranging from 0.4 to
1.2 TeV, is used in the search to discriminate signal from
background processes. No significant deviation from the
Standard Model expectation is observed, and limits are set
on the [Formula: see text] cross-section times branching
ratio. The results are also interpreted as limits on the
<i>QWb</i> coupling and the mixing with the Standard Model
sector for a singlet <i>T</i> quark or a <i>Y</i> quark from
a doublet. <i>T</i> quarks with masses below 0.95 TeV are
excluded at 95 % confidence level, assuming a unit coupling
and a BR[Formula: see text], whereas the expected limit is
1.10 TeV.},
Doi = {10.1140/epjc/s10052-016-4281-8},
Key = {fds321177}
}
@article{fds308492,
Author = {Aaltonen, and T, and others},
Title = {Search for single top quark production in $\bar{p} p$
collisions at $\sqrt{s} = 1.96$ TeV in the missing
transverse energy plus jets topology},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.072003},
Abstract = {http://arxiv.org/abs/1001.4577},
Doi = {10.1103/PhysRevD.81.072003},
Key = {fds308492}
}
@article{fds308763,
Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Amaral, P and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and de
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl,
A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett,
K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan,
AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung,
JY and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly,
A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R and Dagenhart, D},
Title = {Search for single-top-quark production in [Formula
Presented] collisions at [Formula Presented]},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {65},
Number = {9},
Pages = {6},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.65.091102},
Abstract = {We search for standard model single-top-quark production in
the W-gluon fusion and (Formula presented) channels using
(Formula presented) of data from (Formula presented)
collisions at (Formula presented) collected with the
Collider Detector at Fermilab. We set an upper limit at
(Formula presented) confidence level (C.L.) on the combined
W-gluon fusion and (Formula presented) single-top cross
section of 14 pb, roughly six times larger than the standard
model prediction. Separate (Formula presented) C.L. upper
limits in the W-gluon fusion and (Formula presented)
channels are also determined and are found to be 13 and 18
pb, respectively. © 2002 The American Physical
Society.},
Doi = {10.1103/PhysRevD.65.091102},
Key = {fds308763}
}
@article{fds376412,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
Title = {Search for squarks and gluinos in events with hadronically
decaying tau leptons, jets and missing transverse momentum
in proton-proton collisions at [Formula: see text] TeV
recorded with the ATLAS detector.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {12},
Pages = {683},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4481-2},
Abstract = {A search for supersymmetry in events with large missing
transverse momentum, jets, and at least one hadronically
decaying tau lepton has been performed using
3.2 fb[Formula: see text] of proton-proton collision data
at [Formula: see text] recorded by the ATLAS detector at the
Large Hadron Collider in 2015. Two exclusive final states
are considered, with either exactly one or at least two tau
leptons. No excess over the Standard Model prediction is
observed in the data. Results are interpreted in the context
of gauge-mediated supersymmetry breaking and a simplified
model of gluino pair production with tau-rich cascade
decays, substantially improving on previous limits. In the
GMSB model considered, supersymmetry-breaking scale
([Formula: see text]) values below [Formula: see text] are
excluded at the 95% confidence level, corresponding to
gluino masses below [Formula: see text]. For large values of
[Formula: see text], values of [Formula: see text] up to
[Formula: see text] and gluino masses up to [Formula: see
text] are excluded. In the simplified model, gluino masses
are excluded up to [Formula: see text] for neutralino masses
around [Formula: see text]. Neutralino masses below
[Formula: see text] are excluded for all gluino masses
between 800 and [Formula: see text], while the strongest
exclusion of [Formula: see text] is achieved for gluino
masses around [Formula: see text].},
Doi = {10.1140/epjc/s10052-016-4481-2},
Key = {fds376412}
}
@article{fds321259,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
M},
Title = {Search for squarks and gluinos in events with isolated
leptons, jets and missing transverse momentum at √s = 8
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {4},
Publisher = {Springer Nature},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2015)116},
Abstract = {The results of a search for supersymmetry in final states
containing at least one isolated lepton (electron or muon),
jets and large missing transverse momentum with the ATLAS
detector at the Large Hadron Collider are reported. The
search is based on proton-proton collision data at a
centre-of-mass energy √ = 8 TeV collected in 2012,
corresponding to an integrated luminosity of 20 fb−1. No
significant excess above the Standard Model expectation is
observed. Limits are set on supersymmetric particle masses
for various supersymmetric models. Depending on the model,
the search excludes gluino masses up to 1.32 TeV and squark
masses up to 840 GeV. Limits are also set on the parameters
of a minimal universal extra dimension model, excluding a
compactification radius of 1/Rc = 950 GeV for a cut-off
scale times radius (ΛRc) of approximately
30.},
Doi = {10.1007/JHEP04(2015)116},
Key = {fds321259}
}
@article{fds321188,
Author = {Atlas Collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
Kuutmann, E and Berger, N and Beringer, J and Berlendis, S and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro,
R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero,
J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {Search for squarks and gluinos in final states with jets and
missing transverse momentum at [Formula: see text] =13
[Formula: see text]with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {7},
Pages = {392},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4184-8},
Abstract = {A search for squarks and gluinos in final states containing
hadronic jets, missing transverse momentum but no electrons
or muons is presented. The data were recorded in 2015 by the
ATLAS experiment in [Formula: see text] proton-proton
collisions at the Large Hadron Collider. No excess above the
Standard Model background expectation was observed in
3.2 [Formula: see text] of analyzed data. Results are
interpreted within simplified models that assume
<i>R</i>-parity is conserved and the neutralino is the
lightest supersymmetric particle. An exclusion limit at the
95 % confidence level on the mass of the gluino is set at
1.51 [Formula: see text] for a simplified model
incorporating only a gluino octet and the lightest
neutralino, assuming the lightest neutralino is massless.
For a simplified model involving the strong production of
mass-degenerate first- and second-generation squarks, squark
masses below 1.03 [Formula: see text] are excluded for a
massless lightest neutralino. These limits substantially
extend the region of supersymmetric parameter space excluded
by previous measurements with the ATLAS detector.},
Doi = {10.1140/epjc/s10052-016-4184-8},
Key = {fds321188}
}
@article{fds365414,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for squarks and gluinos in final states with jets and
missing transverse momentum using 139 fb −1 of
√s = 13 TeV pp collision data with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {2},
Year = {2021},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2021)143},
Abstract = {A search for the supersymmetric partners of quarks and
gluons (squarks and gluinos) in final states containing jets
and missing transverse momentum, but no electrons or muons,
is presented. The data used in this search were recorded by
the ATLAS experiment in proton-proton collisions at a
centre-of-mass energy of s = 13 TeV during Run 2 of the
Large Hadron Collider, corresponding to an integrated
luminosity of 139 fb−1. The results are interpreted in the
context of various R-parity-conserving models where squarks
and gluinos are produced in pairs or in association and a
neutralino is the lightest supersymmetric particle. An
exclusion limit at the 95% confidence level on the mass of
the gluino is set at 2.30 TeV for a simplified model
containing only a gluino and the lightest neutralino,
assuming the latter is massless. For a simplified model
involving the strong production of mass-degenerate first-
and second-generation squarks, squark masses below 1.85 TeV
are excluded if the lightest neutralino is massless. These
limits extend substantially beyond the region of
supersymmetric parameter space excluded previously by
similar searches with the ATLAS detector. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP02(2021)143},
Key = {fds365414}
}
@article{fds365386,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for squarks and gluinos in final states with one
isolated lepton, jets, and missing transverse momentum at
√s=13 with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09344-w},
Abstract = {The results of a search for gluino and squark pair
production with the pairs decaying via the lightest
charginos into a final state consisting of two W bosons, the
lightest neutralinos (χ~10), and quarks, are presented: the
signal is characterised by the presence of a single charged
lepton (e± or μ±) from a W boson decay, jets, and missing
transverse momentum. The analysis is performed using
139 fb- 1 of proton–proton collision data taken at a
centre-of-mass energy s=13 delivered by the Large Hadron
Collider and recorded by the ATLAS experiment. No
statistically significant excess of events above the
Standard Model expectation is found. Limits are set on the
direct production of squarks and gluinos in simplified
models. Masses of gluino (squark) up to 2.2 (1.4) are
excluded at 95% confidence level for a light
χ~10.},
Doi = {10.1140/epjc/s10052-021-09344-w},
Key = {fds365386}
}
@article{fds321336,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for squarks and gluinos with the ATLAS detector in
final states with jets and missing transverse momentum using
√s = 8 TeV proton-proton collision data},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {9},
Publisher = {Springer Nature},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2014)176},
Abstract = {A search for squarks and gluinos in final states containing
high-pTjets, missing transverse momentum and no electrons or
muons is presented. The data were recorded in 2012 by the
ATLAS experiment in √s = 8TeV proton-proton collisions at
the Large Hadron Collider, with a total integrated
luminosity of 20.3 fb−1. Results are interpreted in a
variety of simplified and specific supersymmetry-breaking
models assuming that R-parity is conserved and that the
lightest neutralino is the lightest supersymmetric particle.
An exclusion limit at the 95% confidence level on the mass
of the gluino is set at 1330GeV for a simplified model
incorporating only a gluino and the lightest neutralino. For
a simplified model involving the strong production of first-
and second-generation squarks, squark masses below 850GeV
(440GeV) are excluded for a massless lightest neutralino,
assuming mass degenerate (single light-flavour) squarks. In
mSUGRA/CMSSM models with tan β = 30, A0= −2m0and μ > 0,
squarks and gluinos of equal mass are excluded for masses
below 1700GeV. Additional limits are set for non-universal
Higgs mass models with gaugino mediation and for simplified
models involving the pair production of gluinos, each
decaying to a top squark and a top quark, with the top
squark decaying to a charm quark and a neutralino. These
limits extend the region of supersymmetric parameter space
excluded by previous searches with the ATLAS
detector.},
Doi = {10.1007/JHEP09(2014)176},
Key = {fds321336}
}
@article{fds314155,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
Title = {Search for standard model Higgs boson production in
association with a W boson at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {78},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2008},
Month = {August},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.78.032008},
Abstract = {We present a search for standard model Higgs boson
production in association with a W boson in
proton-antiproton collisions (pp̄→ W±H→ νbb̄) at a
center of mass energy of 1.96 TeV. The search employs data
collected with the CDF II detector which correspond to an
integrated luminosity of approximately 1fb-1. We select
events consistent with a signature of a single lepton
(e±/μ±), missing transverse energy, and two jets. Jets
corresponding to bottom quarks are identified with a
secondary vertex tagging method and a neural network filter
technique. The observed number of events and the dijet mass
distributions are consistent with the standard model
background expectations, and we set 95% confidence level
upper limits on the production cross section times branching
ratio ranging from 3.9 to 1.3 pb for Higgs boson masses from
110 to 150GeV/c2, respectively. © 2008 The American
Physical Society.},
Doi = {10.1103/PhysRevD.78.032008},
Key = {fds314155}
}
@article{fds308405,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci,
MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
Title = {Search for standard model Higgs boson production in
association with a W boson using a matrix element technique
at CDF in pp̄ collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.85.072001},
Abstract = {This paper presents a search for standard model Higgs boson
production in association with a W boson using events
recorded by the CDF experiment in a data set corresponding
to an integrated luminosity of 5.6fb -1. The search is
performed using a matrix element technique in which the
signal and background hypotheses are used to create a
powerful discriminator. The discriminant output
distributions for signal and background are fit to the
observed events using a binned likelihood approach to search
for the Higgs boson signal. We find no evidence for a Higgs
boson, and 95% confidence level (C.L.) upper limits are set
on σ(pp̄→WH)×B(H→bb̄). The observed limits range
from 3.5 to 37.6 relative to the standard model expectation
for Higgs boson masses between m H=100GeV/c2 and m
H=150GeV/c2. The 95% C.L. expected limit is estimated from
the median of an ensemble of simulated experiments and
varies between 2.9 and 32.7 relative to the production rate
predicted by the standard model over the Higgs boson mass
range studied. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.85.072001},
Key = {fds308405}
}
@article{fds308569,
Author = {Aaltonen, T and others},
Title = {Search for standard model Higgs boson production in
association with a W boson using a neural network
discriminant at CDF},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {1},
Pages = {012002},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.012002},
Abstract = {We present a search for standard model Higgs boson
production in association with a W boson in
proton-antiproton collisions (pp̅ →W ±
H→ℓνbb̅ ) at a center of mass energy of 1.96 TeV. The
search employs data collected with the CDF II detector that
correspond to an integrated luminosity of approximately
1.9 fb-1. We select events consistent with a signature
of a single charged lepton (e ± /μ ± ),
missing transverse energy, and two jets. Jets corresponding
to bottom quarks are identified with a secondary vertex
tagging method, a jet probability tagging method, and a
neural network filter. We use kinematic information in an
artificial neural network to improve discrimination between
signal and background compared to previous analyses. The
observed number of events and the neural network output
distributions are consistent with the standard model
background expectations, and we set 95% confidence level
upper limits on the production cross section times branching
fraction ranging from 1.2 to 1.1 pb or 7.5 to 102 times the
standard model expectation for Higgs boson masses from 110
to 150 GeV/c2, respectively.},
Doi = {10.1103/PhysRevD.80.012002},
Key = {fds308569}
}
@article{fds314176,
Author = {The, ATLASC and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek,
S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J},
Title = {Search for strong production of supersymmetric particles in
final states with missing transverse momentum and at least
three b-jets at (formula presented) TeV proton-proton
collisions with the ATLAS detector},
Journal = {Critical Ultrasound Journal},
Volume = {2014},
Number = {10},
Year = {2014},
Month = {January},
ISSN = {1126-6708},
url = {http://dx.doi.org/10.1007/JHEP10(2014)024},
Abstract = {© 2014, The Author(s). Abstract: This paper reports the
results of a search for strong production of supersymmetric
particles in 20.1 fb−1 of proton-proton collisions at a
centre-of-mass energy of 8 TeV using the ATLAS detector at
the LHC. The search is performed separately in events with
either zero or at least one high-pT lepton (electron or
muon), large missing transverse momentum, high jet
multiplicity and at least three jets identified as
originated from the fragmentation of a b-quark. No excess is
observed with respect to the Standard Model predictions. The
results are interpreted in the context of several
supersymmetric models involving gluinos and scalar top and
bottom quarks, as well as a mSUGRA/CMSSM model. Gluino
masses up to 1340 GeV are excluded, depending on the model,
significantly extending the previous ATLAS
limits.},
Doi = {10.1007/JHEP10(2014)024},
Key = {fds314176}
}
@article{fds308725,
Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
J and Culbertson, R and Dagenhart, D and D'Auria, S and De Barbaro and P and De Cecco and S and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi,
C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede,
S},
Title = {Search for supersymmetric Higgs bosons in the di-tau decay
mode in pp̄ collisions at s=1.8TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {72},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.72.072004},
Abstract = {A search for the direct production of Higgs bosons in the
di-tau decay mode is performed with 86.3±3.5pb-1 of data
collected with the Collider Detector at Fermilab during the
1994-1995 data taking period of the Tevatron. We search for
events where one tau decays to an electron plus neutrinos
and the other tau decays hadronically. We perform a counting
experiment and set limits on the cross section for
supersymmetric Higgs boson production where tan β is large
and mA is small. For a benchmark parameter space point where
mA0=100GeV/c2 and tan β=50, we limit the production cross
section multiplied by the branching ratio to be less than
77.9 pb at the 95% confidence level compared to the
theoretically predicted value of 11.0 pb. This is the first
search for Higgs bosons decaying to tau pairs at a hadron
collider. © 2005 The American Physical Society.},
Doi = {10.1103/PhysRevD.72.072004},
Key = {fds308725}
}
@article{fds315956,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Search for supersymmetry at [Formula: see text] TeV in
final states with jets and two same-sign leptons or three
leptons with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {259},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4095-8},
Abstract = {A search for strongly produced supersymmetric particles is
conducted using signatures involving multiple energetic jets
and either two isolated leptons (<i>e</i> or [Formula: see
text]) with the same electric charge or at least three
isolated leptons. The search also utilises <i>b</i>-tagged
jets, missing transverse momentum and other observables to
extend its sensitivity. The analysis uses a data sample of
proton-proton collisions at [Formula: see text] TeV
recorded with the ATLAS detector at the Large Hadron
Collider in 2015 corresponding to a total integrated
luminosity of 3.2 fb[Formula: see text]. No significant
excess over the Standard Model expectation is observed. The
results are interpreted in several simplified supersymmetric
models and extend the exclusion limits from previous
searches. In the context of exclusive production and
simplified decay modes, gluino masses are excluded at
[Formula: see text] confidence level up to 1.1-1.3 TeV for
light neutralinos (depending on the decay channel), and
bottom squark masses are also excluded up to 540 GeV. In the
former scenarios, neutralino masses are also excluded up to
550-850 GeV for gluino masses around 1 TeV.},
Doi = {10.1140/epjc/s10052-016-4095-8},
Key = {fds315956}
}
@article{fds321349,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Coutinho, YA and Amelung,
C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for supersymmetry at √s= 8 TeV in final states with
jets and two same-sign leptons or three leptons with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {6},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP06(2014)035},
Abstract = {A search for strongly produced supersymmetric particles is
conducted using signatures involving multiple energetic jets
and either two isolated leptons (e or μ) with the same
electric charge, or at least three isolated leptons. The
search also utilises jets originating from b-quarks, missing
transverse momentum and other observables to extend its
sensitivity. The analysis uses a data sample corresponding
to a total integrated luminosity of 20.3 fb-1 of √s = 8
TeV proton-proton collisions recorded with the ATLAS
detector at the Large Hadron Collider in 2012. No deviation
from the Standard Model expectation is observed. New or
significantly improved exclusion limits are set on a wide
variety of supersymmetric models in which the lightest
squark can be of the first, second or third generations, and
in which R-parity can be conserved or violated. [Figure not
available: see fulltext.] © 2014 The Author(s).},
Doi = {10.1007/JHEP06(2014)035},
Key = {fds321349}
}
@article{fds321165,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M},
Title = {Search for supersymmetry in a final state containing two
photons and missing transverse momentum in [Formula: see
text] = 13 TeV [Formula: see text] collisions at the LHC
using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {9},
Pages = {517},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4344-x},
Abstract = {A search has been made for supersymmetry in a final state
containing two photons and missing transverse momentum using
the ATLAS detector at the Large Hadron Collider. The search
makes use of [Formula: see text] of proton-proton collision
data collected at a centre-of-mass energy of 13 TeV in
2015. Using a combination of data-driven and
Monte-Carlo-based approaches, the Standard Model background
is estimated to be [Formula: see text] events. No events are
observed in the signal region; considering the expected
background and its uncertainty, this observation implies a
model-independent 95 % CL upper limit of 0.93 fb (3.0
events) on the visible cross section due to physics beyond
the Standard Model. In the context of a generalized model of
gauge-mediated supersymmetry breaking with a bino-like
next-to-lightest supersymmetric particle, this leads to a
lower limit of 1650 GeV on the mass of a degenerate octet
of gluino states, independent of the mass of the lighter
bino-like neutralino.},
Doi = {10.1140/epjc/s10052-016-4344-x},
Key = {fds321165}
}
@article{fds321297,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
C},
Title = {Search for supersymmetry in events containing a same-flavour
opposite-sign dilepton pair, jets, and large missing
transverse momentum in [Formula: see text] TeV pp
collisions with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {318},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3518-2},
Abstract = {Two searches for supersymmetric particles in final states
containing a same-flavour opposite-sign lepton pair, jets
and large missing transverse momentum are presented. The
proton-proton collision data used in these searches were
collected at a centre-of-mass energy [Formula: see
text] TeV by the ATLAS detector at the Large Hadron
Collider and corresponds to an integrated luminosity of
20.3 fb[Formula: see text]. Two leptonic production
mechanisms are considered: decays of squarks and gluinos
with <i>Z</i> bosons in the final state, resulting in a peak
in the dilepton invariant mass distribution around the
<i>Z</i>-boson mass; and decays of neutralinos (e.g.
[Formula: see text]), resulting in a kinematic endpoint in
the dilepton invariant mass distribution. For the former, an
excess of events above the expected Standard Model
background is observed, with a significance of three
standard deviations. In the latter case, the data are
well-described by the expected Standard Model background.
The results from each channel are interpreted in the context
of several supersymmetric models involving the production of
squarks and gluinos.},
Doi = {10.1140/epjc/s10052-015-3518-2},
Key = {fds321297}
}
@article{fds365388,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for supersymmetry in events with four or more charged
leptons in 139 fb −1 of √s = 13 TeV pp
collisions with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2021)167},
Abstract = {A search for supersymmetry in events with four or more
charged leptons (electrons, muons and τ-leptons) is
presented. The analysis uses a data sample corresponding to
139 fb−1 of proton-proton collisions delivered by the
Large Hadron Collider at s = 13 TeV and recorded by the
ATLAS detector. Four-lepton signal regions with up to two
hadronically decaying τ-leptons are designed to target
several supersymmetric models, while a general five-lepton
signal region targets any new physics phenomena leading to a
final state with five charged leptons. Data yields are
consistent with Standard Model expectations and results are
used to set upper limits on contributions from processes
beyond the Standard Model. Exclusion limits are set at the
95% confidence level in simplified models of general
gauge-mediated supersymmetry, excluding higgsino masses up
to 540 GeV. In R-parity-violating simplified models with
decays of the lightest supersymmetric particle to charged
leptons, lower limits of 1.6 TeV, 1.2 TeV, and 2.5 TeV are
placed on wino, slepton and gluino masses, respectively.
[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP07(2021)167},
Key = {fds365388}
}
@article{fds321330,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for supersymmetry in events with four or more leptons
in √s =8 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.90.052001},
Abstract = {Results from a search for supersymmetry in events with four
or more leptons including electrons, muons and taus are
presented. The analysis uses a data sample corresponding to
20.3 fb-1 of proton-proton collisions delivered by the Large
Hadron Collider at s=8 TeV and recorded by the ATLAS
detector. Signal regions are designed to target
supersymmetric scenarios that can be either enriched in or
depleted of events involving the production of a Z boson. No
significant deviations are observed in data from standard
model predictions and results are used to set upper limits
on the event yields from processes beyond the standard
model. Exclusion limits at the 95% confidence level on the
masses of relevant supersymmetric particles are obtained. In
R-parity-violating simplified models with decays of the
lightest supersymmetric particle to electrons and muons,
limits of 1350 and 750 GeV are placed on gluino and chargino
masses, respectively. In R-parity-conserving simplified
models with heavy neutralinos decaying to a massless
lightest supersymmetric particle, heavy neutralino masses up
to 620 GeV are excluded. Limits are also placed on other
supersymmetric scenarios.},
Doi = {10.1103/PhysRevD.90.052001},
Key = {fds321330}
}
@article{fds325313,
Author = {The ATLAS collaboration and A and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Search for supersymmetry in events with large missing
transverse momentum, jets, and at least one tau lepton in 20
fb−1 of √s= 8 TeV proton-proton collision data with the
ATLAS detector},
Journal = {Social Psychiatry and Psychiatric Epidemiology},
Volume = {2014},
Number = {9},
Publisher = {Dr. Dietrich Steinkopff Verlag GmbH and Co.
KG},
Year = {2014},
url = {http://dx.doi.org/10.1007/JHEP09(2014)103},
Abstract = {A search for supersymmetry (SUSY) in events with large
missing transverse momentum, jets, at least one hadronically
decaying tau lepton and zero or one additional light leptons
(electron/muon), has been performed using 20.3fb−1of
proton-proton collision data at √ s= 8 TeV recorded with
the ATLAS detector at the Large Hadron Collider. No excess
above the Standard Model background expectation is observed
in the various signal regions and 95% confidence level upper
limits on the visible cross section for new phenomena are
set. The results of the analysis are interpreted in several
SUSY scenarios, significantly extending previous limits
obtained in the same final states. In the framework of
minimal gauge-mediated SUSY breaking models, values of the
SUSY breaking scale Λ below 63 TeV are excluded,
independently of tan β. Exclusion limits are also derived
for an mSUGRA/CMSSM model, in both the R-parity-conserving
and R-parity-violating case. A further interpretation is
presented in a framework of natural gauge mediation, in
which the gluino is assumed to be the only light coloured
sparticle and gluino masses below 1090 GeV are
excluded.},
Doi = {10.1007/JHEP09(2014)103},
Key = {fds325313}
}
@article{fds308375,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Saavedra, JAA and Agustoni, M and Aharrouche,
M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Spiers, SEA and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik,
E},
Title = {Search for supersymmetry in events with large missing
transverse momentum, jets, and at least one tau lepton in 7
TeV proton-proton collision data with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {72},
Number = {11},
Publisher = {Springer Nature},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2215-7},
Abstract = {A search for supersymmetry (SUSY) in events with large
missing transverse momentum, jets, and at least one
hadronically decaying τ lepton, with zero or one additional
light lepton (e/μ), has been performed using 4.7 fb−1of
proton-proton collision data at √s = 7 TeV recorded with
the ATLAS detector at the Large Hadron Collider. No excess
above the Standard Model background expectation is observed
and a 95 % confidence level visible cross-section upper
limit for new phenomena is set. In the framework of
gauge-mediated SUSY-breaking models, lower limits on the
mass scale Λ are set at 54 TeV in the regions where the
τ1is the next-to-lightest SUSY particle (tanβ > 20). These
limits provide the most stringent tests to date of GMSB
models in a large part of the parameter space
considered.},
Doi = {10.1140/epjc/s10052-012-2215-7},
Key = {fds308375}
}
@article{fds308347,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, L and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos,
S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JJB and Badescu, E and Bagnaia, P and Bahinipati,
S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio,
EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
Costa, JBG and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Harpaz,
SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni,
A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez,
AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi,
G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
Title = {Search for supersymmetry in events with photons, bottom
quarks, and missing transverse momentum in proton-proton
collisions at a centre-of-mass energy of 7 TeV with the
ATLAS detector},
Journal = {PHYSICS LETTERS B},
Volume = {719},
Number = {4-5},
Pages = {261-279},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.041},
Abstract = {© 2013 CERN A search has been performed for the
experimental signature of an isolated photon with high
transverse momentum, at least one jet identified as
originating from a bottom quark, and high missing transverse
momentum. Such a final state may originate from
supersymmetric models with gauge-mediated supersymmetry
breaking in events in which one of a pair of higgsino-like
neutralinos decays into a photon and a gravitino while the
other decays into a Higgs boson and a gravitino. The search
is performed using the full dataset of 7 TeV proton–proton
collisions recorded with the ATLAS detector at the LHC in
2011, corresponding to an integrated luminosity of 4.7
fb−1. A total of 7 candidate events are observed while
7.5±2.2 events are expected from the Standard Model
background. The results of the search are interpreted in the
context of general gauge mediation to exclude certain
regions of a benchmark plane for higgsino-like neutralino
production.},
Doi = {10.1016/j.physletb.2013.01.041},
Key = {fds308347}
}
@article{fds375939,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Search for supersymmetry in final states with missing
transverse momentum and three or more b-jets in 139
fb-1 of proton–proton collisions at √s=13 TeV
with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11543-6},
Abstract = {A search for supersymmetry involving the pair production of
gluinos decaying via off-shell third-generation squarks into
the lightest neutralino (χ~10) is reported. It exploits LHC
proton–proton collision data at a centre-of-mass energy
s=13 TeV with an integrated luminosity of 139 fb - 1
collected with the ATLAS detector from 2015 to 2018. The
search uses events containing large missing transverse
momentum, up to one electron or muon, and several energetic
jets, at least three of which must be identified as
containing b-hadrons. Both a simple kinematic event
selection and an event selection based upon a deep
neural-network are used. No significant excess above the
predicted background is found. In simplified models
involving the pair production of gluinos that decay via
off-shell top (bottom) squarks, gluino masses less than
2.44 TeV (2.35 TeV) are excluded at 95% CL for a massless
χ~10. Limits are also set on the gluino mass in models with
variable branching ratios for gluino decays to
bb¯χ~10,tt¯χ~10 and tb¯χ~1-/t¯bχ~1+.},
Doi = {10.1140/epjc/s10052-023-11543-6},
Key = {fds375939}
}
@article{fds308573,
Author = {Aaltonen, T and others},
Title = {Search for Supersymmetry in pp̅ Collisions at √ s
=1.96 TeV Using the Trilepton Signature for
Chargino-Neutralino Production},
Journal = {Physical Review Letters},
Volume = {101},
Number = {25},
Pages = {251801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.251801},
Abstract = {We use the three lepton and missing energy trilepton
signature to search for chargino-neutralino production with
2.0 fb-1 of integrated luminosity collected by the CDF
II experiment at the Tevatron pp̅ collider. We expect an
excess of approximately 11 supersymmetric events for a
choice of parameters of the mSUGRA model, but our
observation of 7 events is consistent with the standard
model expectation of 6.4 events. We constrain the mSUGRA
model of supersymmetry and rule out chargino masses up to
145 GeV/c2 for a specific choice of
parameters.},
Doi = {10.1103/physrevlett.101.251801},
Key = {fds308573}
}
@article{fds308487,
Author = {Aaltonen, and T, and others},
Title = {Search for Supersymmetry with Gauge-Mediated Breaking in
Diphoton Events with Missing Transverse Energy at CDF
II},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {1},
Pages = {011801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.011801},
Abstract = {http://arxiv.org/abs/0910.3606},
Doi = {10.1103/PhysRevLett.104.011801},
Key = {fds308487}
}
@article{fds308366,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and d'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucà, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Search for supersymmetry with like-sign lepton-tau events at
CDF.},
Journal = {Physical review letters},
Volume = {110},
Number = {20},
Pages = {201802},
Year = {2013},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.110.201802},
Abstract = {We present a search for chargino-neutralino associated
production using like electric charge dilepton events
collected by the CDF II detector at the Fermilab Tevatron in
proton-antiproton collisions at sqrt[s] = 1.96 TeV. One
lepton is identified as the hadronic decay of a tau lepton,
while the other is an electron or muon. In data
corresponding to 6.0 fb(-1) of integrated luminosity, we
obtain good agreement with standard model predictions and
set limits on the chargino-neutralino production cross
section for simplified gravity- and gauge-mediated models.
As an example, assuming that the chargino and neutralino
decays to taus dominate, in the simplified gauge-mediated
model we exclude cross sections greater than 300 fb at 95%
credibility level for chargino and neutralino masses of 225
GeV/c(2). This analysis is the first to extend the LHC
searches for electroweak supersymmetric production of
gauginos to high tanβ and slepton next-to-lightest
supersymmetric particle scenarios.},
Doi = {10.1103/physrevlett.110.201802},
Key = {fds308366}
}
@article{fds308481,
Author = {Aaltonen, and T, and others},
Title = {Search for Technicolor Particles Produced in Association
with a $W$ Boson at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {11},
Pages = {111802},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.111802},
Abstract = {http://arxiv.org/abs/0912.2059},
Doi = {10.1103/PhysRevLett.104.111802},
Key = {fds308481}
}
@article{fds321159,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for TeV-scale gravity signatures in high-mass final
states with leptons and jets with the ATLAS detector at
√s=13 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {760},
Pages = {520-537},
Publisher = {Elsevier BV},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2016.07.030},
Abstract = {A search for physics beyond the Standard Model, in final
states with at least one high transverse momentum charged
lepton (electron or muon) and two additional high transverse
momentum leptons or jets, is performed using 3.2 fb−1 of
proton–proton collision data recorded by the ATLAS
detector at the Large Hadron Collider in 2015 at s=13 TeV.
The upper end of the distribution of the scalar sum of the
transverse momenta of leptons and jets is sensitive to the
production of high-mass objects. No excess of events beyond
Standard Model predictions is observed. Exclusion limits are
set for models of microscopic black holes with two to six
extra dimensions.},
Doi = {10.1016/j.physletb.2016.07.030},
Key = {fds321159}
}
@article{fds314185,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for the associated production of the Higgs boson with
a top quark pair in multilepton final states with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {749},
Pages = {519-541},
Publisher = {Elsevier BV},
Year = {2015},
Month = {October},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2015.07.079},
Abstract = {A search for the associated production of the Higgs boson
with a top quark pair is performed in multilepton final
states using 20.3 fb−1 of proton–proton collision data
recorded by the ATLAS experiment at s=8 TeV at the Large
Hadron Collider. Five final states, targeting the decays
H→WW⁎, ττ, and ZZ⁎, are examined for the presence of
the Standard Model (SM) Higgs boson: two same-charge light
leptons (e or μ) without a hadronically decaying τ lepton;
three light leptons; two same-charge light leptons with a
hadronically decaying τ lepton; four light leptons; and one
light lepton and two hadronically decaying τ leptons. No
significant excess of events is observed above the
background expectation. The best fit for the tt¯H
production cross section, assuming a Higgs boson mass of 125
GeV, is 2.1−1.2+1.4 times the SM expectation, and the
observed (expected) upper limit at the 95% confidence level
is 4.7 (2.4) times the SM rate. The p-value for
compatibility with the background-only hypothesis is 1.8σ;
the expectation in the presence of a Standard Model signal
is 0.9σ.},
Doi = {10.1016/j.physletb.2015.07.079},
Key = {fds314185}
}
@article{fds308512,
Author = {Aaltonen, T and others},
Title = {Search for the Associated Production of the Standard-Model
Higgs Boson in the All-Hadronic Channel},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {22},
Pages = {221801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.221801},
Abstract = {We report on a search for the standard-model Higgs boson in
pp̅ collisions at sqrt[s]=1.96 TeV using an integrated
luminosity of 2.0 fb-1. We look for production of the
Higgs boson decaying to a pair of bottom quarks in
association with a vector boson V (W or Z) decaying to
quarks, resulting in a four-jet final state. Two of the jets
are required to have secondary vertices consistent with
B-hadron decays. We set the first 95% confidence level upper
limit on the VH production cross section with V(→qq̅
/qq′)H(→bb̅ ) decay for Higgs boson masses of
100--150 GeV/c2 using data from run II at the Fermilab
Tevatron. For mH=120 GeV/c2, we exclude cross sections
larger than 38 times the standard-model prediction.},
Doi = {10.1103/physrevlett.103.221801},
Key = {fds308512}
}
@article{fds321279,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Search for the b¯b decay of the Standard Model Higgs boson
in associated (W/Z)H production with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {1},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2015)069},
Abstract = {Abstract: A search for the (Formula presented.) decay of the
Standard Model Higgs boson is performed with the ATLAS
experiment using the full dataset recorded at the LHC in Run
1. The integrated luminosities used are 4.7 and 20.3 fb−1
from pp collisions at (Formula presented.) and 8 TeV,
respectively. The processes considered are associated (W/Z)H
production, where W → eν/μν, Z → ee/μμ and Z →
νν. The observed (expected) deviation from the
background-only hypothesis corresponds to a significance of
1.4 (2.6) standard deviations and the ratio of the measured
signal yield to the Standard Model expectation is found to
be μ = 0.52 ± 0.32 (stat.) ± 0.24 (syst.) for a Higgs
boson mass of 125.36 GeV. The analysis procedure is
validated by a measurement of the yield of (W/Z)Z production
with (Formula presented.) in the same final states as for
the Higgs boson search, from which the ratio of the observed
signal yield to the Standard Model expectation is found to
be 0.74 ± 0.09 (stat.) ± 0.14 (syst.).[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP01(2015)069},
Key = {fds321279}
}
@article{fds308795,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti,
A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic,
M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell,
M and Caner, A and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang,
PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Ciobanu,
CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli,
M and Costanzo, D and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent,
PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Fiori,
I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch, H and Fukui, Y and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer, S and Giannetti, P and Giromini, P and Glagolev, V and Gold, M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Herndon, M and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Holloway,
L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones,
M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, MJ and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
J and Kordas, K and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen,
AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and IV, AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Loken,
J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari,
L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore,
E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman, J and Nahn, S and Nakada,
H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti,
R and Papadimitriou, V and Pappas, SP and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom,
L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos,
F and Punzi, G and Ragan, K and Rakitine, A and Reher, D and Reichold, A and Riegler, W and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki,
T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton,
P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa, F and Valls, J and III, SV and Velev, G and Vidal, R and Vilar, R and Volobouev,
I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Waters,
D and Watts, T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Search for the charged Higgs boson in the decays of top
quark pairs in the eτ and μτ channels at √s=1.8
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {62},
Number = {1},
Pages = {1-7},
Year = {2000},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.62.012004},
Abstract = {Top quark production offers the unique opportunity to search
for a charged Higgs boson (H±), as the contribution from
t→H+b→τ+νb can be large in extensions of the standard
model. We use results from a search for top quark pair
production by the Collider Detector at Fermilab (CDF) in the
eτ+Slashed E signT+jets and μτ+Slashed E signT+jets
signatures to set an upper limit on the branching ratio of
ℬ(t→H+b) in 106 pb-1 of data. The upper limit is in the
range 0.5 to 0.6 at 95% C.L. for H+ masses in the range 60
to 160 GeV, assuming the branching ratio for H+→τν is
100%. The τ lepton is detected through its 1-prong and
3-prong hadronic decays. ©2000 The American Physical
Society.},
Doi = {10.1103/PhysRevD.62.012004},
Key = {fds308795}
}
@article{fds375927,
Author = {Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Sharma, AS and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Belfkir, M and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Franco, L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo Martinez and N and Portales, L and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Wingerter-Seez, I and Abulaiti, Y and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe,
J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Zhang, J and Berlendis, S and Cheu, E and Delitzsch, CM and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas,
JCJ and De, K and Eifert, T and Farbin, A and Hadavand, HK and Little, JD and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Gazis, EN and Gkountoumis, P and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Perini, L and Tzanis, P and Zacharis, G and Andeen, T and Burton, CD and Choi, K and Nikiforou, N and Onyisi, PUE and Panchal, DK and Roy, A and Unal, M and Webb, AF and Beddall, AJ and Celebi, E},
Title = {Search for the charged-lepton-flavor-violating decay Z →
eμ in pp collisions at √s = 13 TeV ATLAS
detector},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032015},
Abstract = {A search for the charged-lepton-flavor-violating process
Formula Presented is presented, using Formula Presented of
Formula Presented Formula Presented collision data collected
by the ATLAS experiment at the LHC. An excess in the Formula
Presented invariant mass spectrum near the Formula Presented
boson mass would be a striking signature of new physics. No
excess is observed, and an upper limit Formula Presented is
placed on the branching fraction at 95% confidence level,
which is the most stringent limit to date.},
Doi = {10.1103/PhysRevD.108.032015},
Key = {fds375927}
}
@article{fds308760,
Author = {Acosta, D and Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Dominguez,
A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erbacher, R and Errede, D and Errede, S and Fan, Q and Fang, HC and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes,
DW and Giannetti, P and Giordani, MP and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov, I and Goshaw,
AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
J and Heiss, A and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Ivanov, A and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kartal, S and Kasha,
H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim,
MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Lee, AM and Lee, K and Leone, S and Lewis,
JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima,
K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Miyazaki, Y and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Renton, P and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi,
L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt,
MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Sidoti, A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka,
M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi,
K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli,
D and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Tsybychev, D and Turini, N and Ukegawa, F and Vaiciulis, T and Valls, J and Vejcik, S and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar,
R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner,
RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss,
J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli,
S},
Title = {Search for the decay Bs→μ+μ-φ
in pp̄ collisions at √s = 1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {65},
Number = {11},
Pages = {1111011-1111016},
Year = {2002},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.65.111101},
Abstract = {We present a search for the flavor-changing neutral current
decay Bs→μ+μ-φ in pp̄ collisions at √s = 1.8 TeV,
using 91 pb-1 of data collected at the Collider Detector at
Fermilab (CDF). We find two candidate events for this decay,
which are consistent with the background estimate of one
event, and set an upper limit on the branching fraction of
B(Bs→ μ+μ-φ)<6.7×10-5 at a 95% confidence level.
This is the first limit on the branching fraction of this
decay.},
Doi = {10.1103/PhysRevD.65.111101},
Key = {fds308760}
}
@article{fds376249,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Search for the decay of the Higgs boson to a Z boson and a
light pseudoscalar particle decaying to two
photons},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {850},
Year = {2024},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2024.138536},
Abstract = {A search for the decay of the Higgs boson to a Z boson and a
light, pseudoscalar particle, a, decaying respectively to
two leptons and to two photons is reported. The search uses
the full LHC Run 2 proton–proton collision data at s=13
TeV, corresponding to 139 fb−1 collected by the ATLAS
detector. This is one of the first searches for this
specific decay mode of the Higgs boson, and it probes
unexplored parameter space in models with axion-like
particles (ALPs) and extended scalar sectors. The mass of
the a particle is assumed to be in the range 0.1–33 GeV.
The data are analysed in two categories: a merged category
where the photons from the a decay are reconstructed in the
ATLAS calorimeter as a single cluster, and a resolved
category in which two separate photons are detected. The
main background processes are from Standard Model Z boson
production in association with photons or jets. The data are
in agreement with the background predictions, and upper
limits on the branching ratio of the Higgs boson decay to Za
times the branching ratio a→γγ are derived at the 95%
confidence level and they range from 0.08% to 2% depending
on the mass of the a particle. The results are also
interpreted in the context of ALP models.},
Doi = {10.1016/j.physletb.2024.138536},
Key = {fds376249}
}
@article{fds331636,
Author = {Acosta, D and Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D},
Title = {Search for the decay [Formula Presented] in [Formula
Presented] collisions at [Formula Presented]
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {65},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.65.111101},
Abstract = {We present a search for the flavor-changing neutral current
decay [Formula Presented] in [Formula Presented] collisions
at [Formula Presented] using [Formula Presented] of data
collected at the Collider Detector at Fermilab (CDF). We
find two candidate events for this decay, which are
consistent with the background estimate of one event, and
set an upper limit on the branching fraction of [Formula
Presented] at a 95% confidence level. This is the first
limit on the branching fraction of this decay. © 2002 The
American Physical Society.},
Doi = {10.1103/PhysRevD.65.111101},
Key = {fds331636}
}
@article{fds321379,
Author = {Collaboration, CDF},
Title = {Search for the Decays B^0->____ and B^0-> ___ in pp
Collisions at „©s = 1.8 TeV},
Journal = {Phys. Rev. Rapid Communications},
Volume = {D57},
Number = {7},
Pages = {R3811},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevD.57.R3811},
Abstract = {We present a search for the flavor-changing neutral current
decays (Formula presented) and (Formula presented) in
(Formula presented) collisions at (Formula presented) TeV,
using (Formula presented) of data collected at the Collider
Detector at Fermilab. We find one candidate event for these
decays, which is consistent with the background estimates,
and set upper limits on the branching fractions of (Formula
presented) and (Formula presented) at 95% confidence level.
© 1998 The American Physical Society.},
Doi = {10.1103/PhysRevD.57.R3811},
Key = {fds321379}
}
@article{fds308843,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal,
M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli,
M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and Jongh, FD and dell'Agnello, S and dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
R and III, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Nakano, I and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and Compte, TL and Leone, S and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi,
E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Nakada, H and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pondrom,
L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang,
CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli,
S},
Title = {Search for the decays B0d→μ+μ-
and B0s→μ+μ-
in pp̄ collisions at √s=1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {57},
Number = {7},
Pages = {R3811-R3816},
Year = {1998},
ISSN = {0556-2821},
Abstract = {We present a search for the flavor-changing neutral current
decays B0d→μ+μ- and B0s→μ+μ- in pp̄ collisions at
√s=1.8 TeV, using 98 pb-1 of data collected at the
Collider Detector at Fermilab. We find one candidate event
for these decays, which is consistent with the background
estimates, and set upper limits on the branching fractions
of ℬ(B0d→μ+μ -)<8.6×10-7 and ℬ(B0s→μ+μ
-)<2.6×10-6 at 95% confidence level.},
Key = {fds308843}
}
@article{fds308826,
Author = {al, FAE},
Title = {Search for the Decays B^0s,B^0d -> e+u+and Pati-Salam
Leptoquarks},
Journal = {Physical Review Letters},
Volume = {81},
Number = {26},
Pages = {5742},
Year = {1998},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.5742},
Abstract = {We have searched for the decays Bs0 → e±μ∓ and Bd0 →
e±μ∓ using a 102 pb-1 data sample of pp̄ collisions at
√s = 1.8 TeV collected with the Collider Detector at
Fermilab. We set upper limits on the branching fractions of
B(Bs0 → e±μ∓) < 6.1(8.2) × 10-6 and B(Bs0 →
e±μ∓) < 3.5(4.5) × 10-6 at 90(95)% confidence level.
Using these limits, we set lower bounds on the corresponding
Pati-Salam leptoquark masses and find that MLQ(BS0) >
20.7(19.3) TeV/c2 and MLQ(Bd0) > 21.7(20.4) TeV/c2 at
90(95)% confidence level.},
Doi = {10.1103/PhysRevLett.81.5742},
Key = {fds308826}
}
@article{fds308526,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni,
GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest,
R and Frank, MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto,
WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla,
A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D},
Title = {Search for the decays B_{(s)};{0} --> e;{+} micro;{-} and
B_{(s)};{0} --> e;{+} e;{-} in CDF run II.},
Journal = {Physical review letters},
Volume = {102},
Number = {20},
Pages = {201801},
Year = {2009},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.102.201801},
Abstract = {We report results from a search for the lepton flavor
violating decays B_{s};{0} --> e;{+} micro;{-} and B;{0} -->
e;{+} micro;{-}, and the flavor-changing neutral-current
decays B_{s};{0} --> e;{+} e;{-} and B;{0} --> e;{+} e;{-}.
The analysis uses data corresponding to 2 fb;{-1} of
integrated luminosity of pp[over ] collisions at sqrt[s] =
1.96 TeV collected with the upgraded Collider Detector (CDF
II) at the Fermilab Tevatron. The observed number of B0 and
B_{s};{0} candidates is consistent with background
expectations. The resulting Bayesian upper limits on the
branching ratios at 90% credibility level are B(B_{s};{0}
--> e;{+} micro;{-}) < 2.0 x 10;{-7}, B(B;{0} --> e;{+}
micro;{-}) < 6.4 x 10;{-8}, B(B_{s};{0} --> e;{+} e;{-}) <
2.8 x 10;{-7}, and B(B;{0} --> e;{+} e;{-}) < 8.3 x 10;{-8}.
From the limits on B(B_{(s)};{0} --> e;{+} micro;{-}), the
following lower bounds on the Pati-Salam leptoquark masses
are also derived: M_{LQ}(B_{s};{0} --> e;{+} micro;{-}) >
47.8 TeV/c;{2}, and M_{LQ}(B;{0} --> e;{+} micro;{-}) > 59.3
TeV / c;{2}, at 90% credibility level.},
Doi = {10.1103/physrevlett.102.201801},
Key = {fds308526}
}
@article{fds314177,
Author = {The, ATLASC and Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J},
Title = {Search for the direct production of charginos, neutralinos
and staus in final states with at least two hadronically
decaying taus and missing transverse momentum in pp
collisions at √ $$ \sqrt{s}=8 $$ TeV with the ATLAS
detector},
Journal = {Critical Ultrasound Journal},
Volume = {2014},
Number = {10},
Year = {2014},
Month = {January},
ISSN = {1126-6708},
url = {http://dx.doi.org/10.1007/JHEP10(2014)096},
Abstract = {© 2014, The Author(s).Abstract: Results of a search for the
electroweak associated production of charginos and
next-to-lightest neutralinos, pairs of charginos or pairs of
tau sleptons are presented. These processes are
characterised by final states with at least two hadronically
decaying tau leptons, missing transverse momentum and low
jet activity. The analysis is based on an integrated
luminosity of 20.3 fb−1 of proton-proton collisions at
(Formula presented) recorded with the ATLAS experiment at
the Large Hadron Collider. No significant excess is observed
with respect to the predictions from Standard Model
processes. Limits are set at 95% confidence level on the
masses of the lighter chargino and next-to-lightest
neutralino for various hypotheses for the lightest
neutralino mass in simplified models. In the scenario of
direct production of chargino pairs, with each chargino
decaying into the lightest neutralino via an intermediate
tau slepton, chargino masses up to 345 GeV are excluded for
a massless lightest neutralino. For associated production of
mass-degenerate charginos and next-to-lightest neutralinos,
both decaying into the lightest neutralino via an
intermediate tau slepton, masses up to 410 GeV are excluded
for a massless lightest neutralino.[Figure not available:
see fulltext.]},
Doi = {10.1007/JHEP10(2014)096},
Key = {fds314177}
}
@article{fds308577,
Author = {Collaboration, DAEACDF},
Title = {Search for the flavor-changing neutral current decay
D0-->µ+µ- in pp-bar collisions at sqrt[s]=1.96 TeV},
Journal = {Physical Review},
Volume = {D68},
Number = {19},
Pages = {091101},
Year = {2003},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.101.192002},
Abstract = {We report on a search for the flavor-changing neutral
current decay D0-->µ+µ- in pp-bar collisions at
sqrt[s]=1.96 TeV using 65 pb-1 of data collected by the
CDF II experiment at the Fermilab Tevatron Collider. A
displaced-track trigger selects long-lived D0 candidates in
the D0-->µ+µ- search channel, the kinematically similar
D0--> pi + pi - channel used for normalization, the
Cabibbo-favored D0-->K- pi + channel used to optimize the
selection criteria in an unbiased manner, and their charge
conjugates. Finding no signal events in the D0-->µ+µ-
search window, we set an upper limit on the branching
fractionB(D0-- >µ+µ-)},
Doi = {10.1103/physrevlett.101.192002},
Key = {fds308577}
}
@article{fds330939,
Author = {Collaboration, CDF},
Title = {Search for the Flavor-Changing Neutral Current Decays Bƒy
„_ ƒÝƒyƒÝ-Kƒy and B0 „_ ƒÝƒyƒÝ-K*0},
Journal = {Phys. Rev. Lett.},
Volume = {83},
Number = {17},
Pages = {3378},
Publisher = {American Physical Society (APS)},
Year = {1999},
url = {http://dx.doi.org/10.1103/PhysRevLett.83.3378},
Abstract = {We report on a search for the flavor-changing neutral
current decays B+→μ+ μ-K+ and B0→ μ+ μ-K*0 using
88pb-1 of data from p¯p collisions at √s=1.8TeV,
collected with the Collider Detector at Fermilab. Finding no
evidence for these decays, we set upper limits on the
branching fractions B(B+→ μ+ μ-K+)<5.2×10-6 and B(B0→
μ+ μ-K*0)<4.0×10-6 at the 90% confidence level. © 1999
The American Physical Society.},
Doi = {10.1103/PhysRevLett.83.3378},
Key = {fds330939}
}
@article{fds308383,
Author = {Aaltonen, T and González, BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
Title = {Search for the Higgs boson in the all-hadronic final state
using the full CDF data set},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {2},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP02(2013)004},
Abstract = {This paper reports the result of a search for the standard
model Higgs boson in events containing four reconstructed
jets associated with quarks. For masses below 135 GeV/c 2,
the Higgs boson decays to bottom-antibottom quark pairs are
dominant and result primarily in two hadronic jets. An
additional two jets can be produced in the hadronic decay of
a W or Z boson produced in association with the Higgs boson,
or from the incoming quarks that produced the Higgs boson
through the vector-boson fusion process. The search is
performed using a sample of √s=1.96 TeV proton-antiproton
collisions corresponding to an integrated luminosity of 9.45
fb-1 recorded by the CDF II detector. The data are in
agreement with the background model and 95% credibility
level upper limits on Higgs boson production are set as a
function of the Higgs boson mass. The median expected
(observed) limit for a 125 GeV/c 2 Higgs boson is 11.0 (9.0)
times the predicted standard model rate. © 2013
SISSA.},
Doi = {10.1007/JHEP02(2013)004},
Key = {fds308383}
}
@article{fds323482,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli,
A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich,
LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A},
Title = {Search for the Higgs boson produced in association with a W
boson and decaying to four b-quarks via two spin-zero
particles in pp collisions at 13 TeV with the ATLAS
detector.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {11},
Pages = {605},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4418-9},
Abstract = {This paper presents a dedicated search for exotic decays of
the Higgs boson to a pair of new spin-zero particles,
[Formula: see text], where the particle a decays to b-quarks
and has a mass in the range of 20-60 GeV. The search is
performed in events where the Higgs boson is produced in
association with a [Formula: see text] boson, giving rise to
a signature of a lepton (electron or muon), missing
transverse momentum, and multiple jets from b-quark decays.
The analysis is based on the full dataset of pp collisions
at [Formula: see text] recorded in 2015 by the ATLAS
detector at the CERN Large Hadron Collider, corresponding to
an integrated luminosity of 3.2 [Formula: see text]. No
significant excess of events above the Standard Model
prediction is observed, and a [Formula: see text]
confidence-level upper limit is derived for the product of
the production cross section for [Formula: see text] times
the branching ratio for the decay [Formula: see text]. The
upper limit ranges from 6.2 pb for an a-boson mass
[Formula: see text] to 1.5 pb for [Formula: see
text].},
Doi = {10.1140/epjc/s10052-016-4418-9},
Key = {fds323482}
}
@article{fds308575,
Author = {Aaltonen, T and others},
Title = {Search for the Higgs Boson Produced in Association with
Z→ℓ+ℓ- in pp̅ Collisions at sqrt[s] =1.96
TeV},
Journal = {Physical Review Letters},
Volume = {101},
Number = {25},
Pages = {251803},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.251803},
Abstract = {We present a search for the Higgs boson in the process qq̅
→ZH→ℓ+ℓ-bb̅ . The analysis uses an integrated
luminosity of 1 fb-1 of pp̅ collisions produced at
sqrt[s]=1.96 TeV and accumulated by the upgraded
Collider Detector at Fermilab (CDF II). We employ artificial
neural networks both to correct jets mismeasured in the
calorimeter and to distinguish the signal kinematic
distributions from those of the background. We see no
evidence for Higgs boson production, and set 95% C.L. upper
limits on σZHB(H→bb̅ ), ranging from 1.5 to 1.2 pb for a
Higgs boson mass (mH) of 110 to 150 GeV/c2.},
Doi = {10.1103/physrevlett.101.251803},
Key = {fds308575}
}
@article{fds308564,
Author = {Aaltonen, T and others},
Title = {Search for the Higgs boson produced in association with
Z→ℓ+ℓ- using the matrix element method at CDF
II},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {7},
Pages = {071101},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.071101},
Abstract = {We present a search for associated production of the
standard model Higgs boson and a Z boson where the Z boson
decays to two leptons and the Higgs decays to a pair of b
quarks in pp̅ collisions at the Fermilab Tevatron. We use
event probabilities based on standard model matrix elements
to construct a likelihood function of the Higgs content of
the data sample. In a CDF data sample corresponding to an
integrated luminosity of 2.7 fb-1 we see no evidence of
a Higgs boson with a mass between 100 GeV/c2 and
150 GeV/c2. We set 95% confidence level upper limits on
the cross section for ZH production as a function of the
Higgs boson mass mH; the limit is 8.2 times the standard
model prediction at mH=115 GeV/c2.},
Doi = {10.1103/PhysRevD.80.071101},
Key = {fds308564}
}
@article{fds321325,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Djuvsland, JI and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Kucuk, H and Anisenkov,
AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Search for the lepton flavor violating decay Z → eμ in pp
collisions at √s = 8 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.90.072010},
Abstract = {The ATLAS detector at the Large Hadron Collider is used to
search for the lepton flavor violating process Z → eμ in
pp collisions using 20.3 fb-1 of data collected at √s = 8
TeV. An enhancement in the eμ invariant mass spectrum is
searched for at the Z-boson mass. The number of Z bosons
produced in the data sample is estimated using events of
similar topology, Z → ee and μμ, significantly reducing
the systematic uncertainty in the measurement. There is no
evidence of an enhancement at the Z-boson mass, resulting in
an upper limit on the branching fraction, B(Z → 7.5 ×
10.7 at the 95% confidence level.},
Doi = {10.1103/PhysRevD.90.072010},
Key = {fds321325}
}
@article{fds308549,
Author = {Aaltonen, T and others},
Title = {Search for the neutral current top quark decay t→Zc using
the ratio of Z-boson+4 jets to W-boson+4 jets
production},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {5},
Pages = {052001},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.052001},
Abstract = {We have used the Collider Detector at Fermilab (CDF-II) to
search for the flavor-changing neutral-current (FCNC)
top-quark decay t→Zc using a technique employing ratios of
W and Z production, measured in pp̅ data corresponding to
an integrated luminosity of 1.52 fb-1. The analysis
uses a comparison of two decay chains, pp̅ →tt̅
→WbWb→ℓνbjjb and pp̅ →tt̅ →ZcWb→ℓℓcjjb,
to cancel systematic uncertainties in acceptance,
efficiency, and luminosity. We validate the modeling of
acceptance and efficiency for lepton identification over the
multiyear data set using another ratio of W and Z
production, in this case the observed ratio of inclusive
production of W to Z bosons. To improve the discrimination
against standard model backgrounds to top-quark decays, we
calculate the top-quark mass for each event with two leptons
and four jets assuming it is a tt̅ event with one of the
top quarks decaying to Zc. For additional background
discrimination we require at least one jet to be identified
as originating from a b quark. No significant signal is
found and we set an upper limit on the FCNC branching ratio
Br(t→Zc) using a likelihood constructed from the
ℓℓcjjb top-quark mass distribution and the number of
ℓνbjjb events. Limits are set as a function of the
helicity of the Z boson produced in the FCNC decay. For 100%
longitudinally-polarized Z bosons we find limits of 8.3% and
9.3% (95% C.L.) depending on the assumptions regarding the
theoretical top-quark pair production cross
section.},
Doi = {10.1103/PhysRevD.80.052001},
Key = {fds308549}
}
@article{fds308352,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for the neutral Higgs bosons of the minimal
supersymmetric standard model in pp collisions at √s = 7
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {2},
Pages = {1-46},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP02(2013)095},
Abstract = {A search for neutral Higgs bosons of the Minimal
Supersymmetric Standard Model (MSSM) is reported. The
analysis is based on a sample of proton-proton collisions at
a centre-of-mass energy of 7TeV recorded with the ATLAS
detector at the Large Hadron Collider. The data were
recorded in 2011 and correspond to an integrated luminosity
of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into
oppositely-charged muon or τ lepton pairs are considered
for final states requiring either the presence or absence of
b-jets. No statistically significant excess over the
expected background is observed and exclusion limits at the
95% confidence level are derived. The exclusion limits are
for the production cross-section of a generic neutral Higgs
boson, φ, as a function of the Higgs boson mass and for
h/A/H production in the MSSM as a function of the parameters
mA and tan β in the mhmax scenario for mA in the range of
90GeV to 500 GeV. Copyright CERN.},
Doi = {10.1007/JHEP02(2013)095},
Key = {fds308352}
}
@article{fds308521,
Author = {Aaltonen, T and others},
Title = {Search for the Production of Narrow tb̅ Resonances in 1.9
fb-1 of pp̅ Collisions at sqrt[s] =1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {4},
Pages = {041801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.041801},
Abstract = {We present new limits on resonant tb̅ production in pp̅
collisions at sqrt[s]=1.96 TeV, using 1.9 fb-1 of
data recorded with the CDF II detector at the Fermilab
Tevatron. We reconstruct a candidate tb̅ mass in events
with a lepton, neutrino candidate, and two or three jets,
and search for anomalous tb̅ production as modeled by
W′→tb̅ . We set a new limit on a right-handed W′ with
standard model-like coupling, excluding any mass below
800 GeV/c2 at 95% C.L. The cross section for any
narrow, resonant tb̅ production between 750 and
950 GeV/c2 is found to be less than 0.28 pb at 95% C.L.
We also present an exclusion of the W′ coupling strength
versus W′ mass over the range 300--950 GeV/c2.},
Doi = {10.1103/physrevlett.103.041801},
Key = {fds308521}
}
@article{fds308473,
Author = {Aaltonen, and T, and others},
Title = {Search for the Production of Scalar Bottom Quarks in $p
\bar{p}$ collisions at $\sqrt{s} = 1.96$
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {8},
Pages = {081802},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.081802},
Abstract = {http://arxiv.org/abs/1005.3600},
Doi = {10.1103/PhysRevLett.105.081802},
Key = {fds308473}
}
@article{fds308297,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Search for the production of ZW and ZZ boson pairs decaying
into charged leptons and jets in pp̄ collisions at
√s=1.96 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {9},
Pages = {092002},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.88.092002},
Abstract = {We present a measurement of the production cross section for
ZW and ZZ boson pairs in final states with a pair of charged
leptons, from the decay of a Z boson, and at least two jets,
from the decay of a W or Z boson, using the full sample of
proton-antiproton collisions recorded with the CDF II
detector at the Tevatron, corresponding to 8.9 fb-1 of
integrated luminosity. We increase the sensitivity to
vector-boson decays into pairs of quarks using a
neural-network discriminant that exploits the differences
between the spatial spread of energy depositions and
charged-particle momenta contained within the jet of
particles originating from quarks and gluons. Additionally,
we employ new jet energy corrections to Monte Carlo
simulations that account for differences in the observed
energy scales for quark and gluon jets. The number of signal
events is extracted through a simultaneous fit to the dijet
mass spectrum in three classes of events: events likely to
contain jets with a heavy-quark decay, events likely to
contain jets originating from light quarks, and events that
fail these identification criteria. We determine the
production cross section to be σZW+ZZ=2.5-1.0+2.0 pb (<6.1
pb at the 95% confidence level), consistent with the
standard model prediction of 5.1 pb. © 2013 American
Physical Society.},
Doi = {10.1103/PhysRevD.88.092002},
Key = {fds308297}
}
@article{fds331486,
Author = {Collaboration, CDF},
Title = {Search for the Rare Decay W+ ->ƒà+ + ƒ× in
Proton-Antiproton Collisions at = 1.8 TeV},
Journal = {Phys. Rev. Rapid Communications},
Volume = {D58},
Number = {3},
Pages = {031101},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevD.58.031101},
Abstract = {We have searched for the rare decay [Formula Presented] in
[Formula Presented] of data taken in proton-antiproton
collisions at [Formula Presented] with the Collider Detector
at Fermilab. We find three events in the signal region and
estimate the background to be 5.2±1.5 events. We set a 95%
confidence level upper limit of [Formula Presented] on the
ratio of partial widths, [Formula Presented]. © 1998 The
American Physical Society.},
Doi = {10.1103/PhysRevD.58.031101},
Key = {fds331486}
}
@article{fds321380,
Author = {Collaboration, CDF},
Title = {Search for the Rare Decay W+,->D+ pp in Collisions at „©
s= 1.8 TeV},
Journal = {Phys. Rev.},
Volume = {D58},
Number = {9},
Pages = {5},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevD.58.091101},
Abstract = {We search for the rare decay [Formula Presented] in [Formula
Presented] of [Formula Presented] collisions recorded with
the Collider Detector at Fermilab. At the 95% confidence
level, we find an upper limit on the relative branching
fraction to be [Formula Presented]. © 1998 The American
Physical Society.},
Doi = {10.1103/PhysRevD.58.091101},
Key = {fds321380}
}
@article{fds308828,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
R and Engels, E and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch, H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handa,
T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris,
RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Nakano, I and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu,
YC and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martin, A and Matthews,
JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Nakada, H and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg,
D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith,
C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella,
F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka, M and Tannenbaum,
B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto,
Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk,
W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal,
R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson,
R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Search for the rare decay W± →
Dsplusmnγ in pp̄ collisions at √s
= 1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {58},
Number = {9},
Pages = {911011-911015},
Year = {1998},
ISSN = {0556-2821},
Key = {fds308828}
}
@article{fds308888,
Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cen, Y and Cervelli, F and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cunningham, JD and Daniels, T and Jongh, FD and Delchamps, S and dell'Agnello, S and dell'Orso, M and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dickson, M and Dittmann,
JR and Donati, S and Drucker, RB and Dunn, A and Einsweiler, K and Elias,
JE and Ely, R and Jr, EE and Eno, S and Errede, D and Errede, S and Fan, Q and Farhat, B and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman, J and Frisch, H and Fry, A and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro, M and Garfinkel, AF and Geer, S and Gerdes, DW and Giannetti,
P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold, M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Grewal, A and Groer, L and Grosso-Pilcher, C and Haber,
C and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Heinrich, J and Cronin-Hennessy, D and Hollebeek, R and Holloway, L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes,
R and Hurst, P and Huston, J and Huth, J and Hylen, J and Incagli, M and Incandela, J and Iso, H and Jensen, H and Jessop, CP and Joshi, U and Kadel, RW and Kajfasz, E and Kamon, T and Kaneko, T and Kardelis, DA and Kasha, H and Kato, Y and Keeble, L and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and Compte, TL and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Loomis, C and Long, O and Loreti, M and Low, EH and Lu, J and Lucchesi, D and Luchini,
CB and Lukens, P and Lys, J and Maas, P and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Michail, G and Mikamo, S and Miller, M and Miller, R and Mimashi, T and Miscetti, S and Mishina, M and Mitsushio, H and Miyashita, S and Morita, Y and Moulding,
S and Mueller, J and Mukherjee, A and Muller, T and Musgrave, P and Nakae,
LF and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Nodulman, L and Ogawa, S and Oh, SH and Ohl, KE and Oishi, R and Okusawa,
T and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Park, S and Patrick, J and Pauletta, G and Paulini, M and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Plunkett, R and Pondrom, L and Produit, N and Proudfoot, J and Ptohos,
F and Punzi, G and Ragan, K and Rimondi, F and Ristori, L and Roach-Bellino, M and Robertson, WJ and Rodrigo, T and Romano, J and Rosenson, L and Sakumoto, WK and Saltzberg, D and Sansoni, A and Scarpine, V and Schindler, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schneider, O and Sciacca, GF and Scribano, A and Segler,
S and Seidel, S and Seiya, Y and Sganos, G and Sgolacchia, A and Shapiro,
M and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Smith, DA and Snider, FD and Song, L and Song, T and Spalding,
J and Spiegel, L and Sphicas, P and Stanco, L and Steele, J and Stefanini,
A and Strahl, K and Strait, J and Stuart, D and Sullivan, G and Sumorok, K and Swartz, RL and Takahashi, T and Takikawa, K and Tartarelli, F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, J and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov,
A and Tkaczyk, S and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Tseng, J and Turcotte, M and Turini, N and Uemura, N and Ukegawa, F and Unal, G and Brink, SCVD and Vejcik, S and Vidal, R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wainer, N and Walker, RC and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, G and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and III, WCW and Westhusing, T and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer,
BL and Wolinski, J and Wu, DY and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef,
C and Yoshida, T and Yovanovitch, D and Yu, I and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, S and Zhang, W and Zucchelli,
S},
Title = {Search for the rare decay W± → π
± + γ},
Journal = {Physical Review Letters},
Volume = {76},
Number = {16},
Pages = {2852-2857},
Year = {1996},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.76.2852},
Abstract = {We have searched for the rare decay W± → π± + γ in
16.7 pb-1 of data taken in proton-antiproton collisions at
∫s = 1.8 TeV with the CDF detector at Fermilab. We find
one event consistent with the expected signal, and estimate
the background to be 2.6 ± 1.0(stat) ± 1.3(syst) events.
Without background subtraction, we find the ratio of partial
widths to be Γ(W± → π± + γ)/Γ(W± → e± + ν) ≤
2.0 × 103 at the 95% confidence level.},
Doi = {10.1103/physrevlett.76.2852},
Key = {fds308888}
}
@article{fds308541,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
Title = {Search for the rare decays B+→μ+μ-K+, B0→μ+μ-
K*(892)0, and Bs0→μ+μ- at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.79.011104},
Abstract = {We search for b→sμ+μ- transitions in B meson (B+, B0, or
Bs0) decays with 924pb-1 of pp̄ collisions at s=1.96TeV
collected with the CDF II detector at the Fermilab Tevatron.
We find excesses with significances of 4.5, 2.9, and 2.4
standard deviations in the B+→μ+μ-K+,
B0→μ+μ-K*(892)0, and Bs0→μ+μ- decay modes,
respectively. Using B→J/ψh (h=K+, K*(892)0,) decays as
normalization channels, we report branching fractions for
the previously observed B+ and B0 decays,
B(B+→μ+μ-K+)=(0.59±0.15±0. 04)×10-6, and
B(B0→μ+μ-K*(892)0)=(0.81±0. 30±0.10)×10-6, where the
first uncertainty is statistical, and the second is
systematic. We set an upper limit on the relative branching
fraction B(Bs0→μ+μ-)/B(Bs0→J/ψ)<2.6(2.3)×10-3 at the
95(90)% confidence level, which is the most stringent to
date. © 2009 The American Physical Society.},
Doi = {10.1103/PhysRevD.79.011104},
Key = {fds308541}
}
@article{fds308402,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
Title = {Search for the rare radiative decay W→πγ in pp̄
collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.85.032001},
Abstract = {We present a search for the rare radiative decay W ±→ π
±γ using data corresponding to an integrated luminosity of
4.3fb -1 of proton-antiproton collisions at a center-of-mass
energy of 1.96 TeV collected by the CDF experiment at
Fermilab. As no statistically significant signal is
observed, we set a 95%-confidence-level upper limit on the
relative branching fraction Γ(W ±→π ±γ)/Γ(W ±→e
±ν) at 6.4×10 -5, a factor of 10 improvement over the
previous limit. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.85.032001},
Key = {fds308402}
}
@article{fds321355,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for the Standard Model Higgs boson decay to
μ+μ− with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {738},
Number = {1},
Pages = {68-86},
Publisher = {Elsevier BV},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2014.09.008},
Abstract = {A search is reported for Higgs boson decay to μ+μ− using
data with an integrated luminosity of 24.8 fb−1collected
with the ATLAS detector in pp collisions at s=7and8 TeV at
the CERN Large Hadron Collider. The observed dimuon
invariant mass distribution is consistent with the Standard
Model background-only hypothesis in the 120–150 GeV search
range. For a Higgs boson with a mass of 125.5 GeV, the
observed (expected) upper limit at the 95% confidence level
is 7.0 (7.2) times the Standard Model expectation. This
corresponds to an upper limit on the branching ratio
BR(H→μ+μ−) of 1.5×10−3.},
Doi = {10.1016/j.physletb.2014.09.008},
Key = {fds321355}
}
@article{fds321200,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Search for the Standard Model Higgs boson decaying into bb¯
produced in association with top quarks decaying
hadronically in pp collisions at √s = 8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {5},
Publisher = {Springer Nature},
Year = {2016},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2016)160},
Abstract = {A search for Higgs boson production in association with a
pair of top quarks (tt¯ H) is performed, where the Higgs
boson decays to bb¯, and both top quarks decay
hadronically. The data used correspond to an integrated
luminosity of 20.3 fb−1 of pp collisions at √s = 8 TeV
collected with the ATLAS detector at the Large Hadron
Collider. The search selects events with at least six
energetic jets and uses a boosted decision tree algorithm to
discriminate between signal and Standard Model background.
The dominant multijet background is estimated using a
dedicated data-driven technique. For a Higgs boson mass of
125 GeV, an upper limit of 6.4 (5.4) times the Standard
Model cross section is observed (expected) at 95% confidence
level. The best-fit value for the signal strength is μ =
1.6 ± 2.6 times the Standard Model expectation for mH = 125
GeV. Combining all tt¯ H searches carried out by ATLAS at
√s = 8 and 7 TeV, an observed (expected) upper limit of
3.1 (1.4) times the Standard Model expectation is obtained
at 95% confidence level, with a signal strength μ = 1.7 ±
0.8.},
Doi = {10.1007/JHEP05(2016)160},
Key = {fds321200}
}
@article{fds308381,
Author = {Kotwal, AV and Collaboration, CDF},
Title = {Search for the standard model Higgs boson decaying to a
b-bbar pair in events with two oppositely charged leptons
using the full CDF data set},
Journal = {Phys. Rev. Lett.},
Volume = {109},
Number = {11},
Pages = {111803},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.109.111803},
Abstract = {We present a search for the standard model Higgs boson
produced in association with a Z boson in data collected
with the CDF II detector at the Tevatron, corresponding to
an integrated luminosity of 9.45 fb(-1). In events
consistent with the decay of the Higgs boson to a
bottom-quark pair and the Z boson to electron or muon pairs,
we set 95% credibility level upper limits on the ZH
production cross section times the H→bb branching ratio as
a function of Higgs boson mass. At a Higgs boson mass of
125 GeV/c(2), we observe (expect) a limit of 7.1 (3.9)
times the standard model value.},
Doi = {10.1103/physrevlett.109.111803},
Key = {fds308381}
}
@article{fds321371,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
ME and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci,
A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington,
S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest,
R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic,
I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Search for the standard model Higgs boson decaying to a bb
pair in events with no charged leptons and large missing
transverse energy using the full CDF data
set.},
Journal = {Physical review letters},
Volume = {109},
Number = {11},
Pages = {111805},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.109.111805},
Abstract = {We report on a search for the standard model Higgs boson
produced in association with a vector boson in the full data
set of proton-antiproton collisions at sqrt[s]=1.96 TeV
recorded by the CDF II detector at the Tevatron,
corresponding to an integrated luminosity of
9.45 fb(-1). We consider events having no identified
charged lepton, a transverse energy imbalance, and two or
three jets, of which at least one is consistent with
originating from the decay of a b quark. We place 95%
credibility level upper limits on the production cross
section times standard model branching fraction for several
mass hypotheses between 90 and 150 GeV/c(2). For a
Higgs boson mass of 125 GeV/c(2), the observed
(expected) limit is 6.7 (3.6) times the standard model
prediction.},
Doi = {10.1103/physrevlett.109.111805},
Key = {fds321371}
}
@article{fds308382,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
ME and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci,
A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington,
S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeans, DT and Jeon, EJ and Jindariani, S and Jones,
M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi,
A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Search for the standard model Higgs boson decaying to a bb
pair in events with one charged lepton and large missing
transverse energy using the full CDF data
set.},
Journal = {Physical review letters},
Volume = {109},
Number = {11},
Pages = {111804},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.109.111804},
Abstract = {We present a search for the standard model Higgs boson
produced in association with a W boson in
sqrt[s]=1.96 TeV pp collision data collected with the
CDF II detector at the Tevatron corresponding to an
integrated luminosity of 9.45 fb(-1). In events
consistent with the decay of the Higgs boson to a
bottom-quark pair and the W boson to an electron or muon and
a neutrino, we set 95% credibility level upper limits on the
WH production cross section times the H→bb branching ratio
as a function of Higgs boson mass. At a Higgs boson mass of
125 GeV/c(2), we observe (expect) a limit of 4.9 (2.8)
times the standard model value.},
Doi = {10.1103/physrevlett.109.111804},
Key = {fds308382}
}
@article{fds321150,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Search for the Standard Model Higgs boson produced by
vector-boson fusion and decaying to bottom quarks in √s=8
TeV pp collisions with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {11},
Publisher = {Springer Nature},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2016)112},
Abstract = {A search with the ATLAS detector is presented for the
Standard Model Higgs boson produced by vector-boson fusion
and decaying to a pair of bottom quarks, using 20.2 fb−1
of LHC proton-proton collision data at s=8 TeV. The signal
is searched for as a resonance in the invariant mass
distribution of a pair of jets containing b-hadrons in
vector-boson-fusion candidate events. The yield is measured
to be −0.8 ± 2.3 times the Standard Model cross-section
for a Higgs boson mass of 125 GeV. The upper limit on the
cross-section times the branching ratio is found to be 4.4
times the Standard Model cross-section at the 95% confidence
level, consistent with the expected limit value of 5.4 (5.7)
in the background-only (Standard Model production)
hypothesis.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP11(2016)112},
Key = {fds321150}
}
@article{fds316856,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for the standard model Higgs boson produced in
association with a vector boson and decaying into a tau pair
in pp collisions at s =8 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {93},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {May},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.93.092005},
Abstract = {A search for the standard model Higgs boson produced in
association with a vector boson with the decay H→ττ is
presented. The data correspond to 20.3 fb-1 of integrated
luminosity from proton-proton collisions at s=8 TeV recorded
by the ATLAS experiment at the LHC during 2012. The data
agree with the background expectation, and 95%
confidence-level upper limits are placed on the cross
section of this process. The observed (expected) limit,
expressed in terms of the signal strength μ=σ/σSM for
mH=125 GeV, is μ<5.6 (3.7). The measured value of the
signal strength is μ=2.3±1.6.},
Doi = {10.1103/PhysRevD.93.092005},
Key = {fds316856}
}
@article{fds308416,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Search for the standard model Higgs boson produced in
association with a W ± boson with 7.5fb
-1 integrated luminosity at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.86.032011},
Abstract = {We present a search for the standard model Higgs boson
produced in association with a W ± boson. This search uses
data corresponding to an integrated luminosity of 7.5fb -1
collected by the CDF detector at the Tevatron. We select
WH→νbb̄ candidate events with two jets, large missing
transverse energy, and exactly one charged lepton. We
further require that at least one jet be identified to
originate from a bottom quark. Discrimination between the
signal and the large background is achieved through the use
of a Bayesian artificial neural network. The number of
tagged events and their distributions are consistent with
the standard model expectations. We observe no evidence for
a Higgs boson signal and set 95% C.L. upper limits on the WH
production cross section times the branching ratio to decay
to bb̄ pairs, σ(pp̄→W ±H) ×B(H→bb̄), relative to
the rate predicted by the standard model. For the Higgs
boson mass range of 100 to 150GeV/c2 we set observed
(expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For
115GeV/c2 the upper limit is 3.64 (2.78). The combination of
the present search with an independent analysis that selects
events with three jets yields more stringent limits ranging
from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For
115 and 125GeV/c2 the upper limits are 2.65 (2.60) and 4.36
(3.69), respectively. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.032011},
Key = {fds308416}
}
@article{fds308418,
Author = {Kotwal, AV and Collaboration, CDF},
Title = {Search for the standard model Higgs boson produced in
association with a Z boson in 7.9/fb of ppbar collisions at
sqrt(s)=1.96 TeV using the CDF II detector},
Journal = {Phys. Lett. B},
Volume = {715},
Number = {1-3},
Pages = {98},
Publisher = {Elsevier BV},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2012.07.045},
Abstract = {We present a search for the standard model Higgs boson
produced in association with a Z boson, using up to 7.9 fb
-1 of integrated luminosity from pp- collisions collected
with the CDF II detector. We utilize several novel
techniques, including multivariate lepton selection,
multivariate trigger parametrization, and a multi-stage
signal discriminant consisting of specialized functions
trained to distinguish individual backgrounds. By increasing
acceptance and enhancing signal discrimination, these
techniques have significantly improved the sensitivity of
the analysis above what was expected from a larger dataset
alone. We observe no significant evidence for a signal, and
we set limits on the ZH production cross section. For a
Higgs boson with mass 115 GeV/c 2, we expect (observe) a
limit of 3.9 (4.8) times the standard model predicted value,
at the 95% credibility level. © 2012 Elsevier
B.V.},
Doi = {10.1016/j.physletb.2012.07.045},
Key = {fds308418}
}
@article{fds321303,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
C},
Title = {Search for the Standard Model Higgs boson produced in
association with top quarks and decaying into [Formula: see
text] in [Formula: see text] collisions at [Formula: see
text] with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {349},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3543-1},
Abstract = {A search for the Standard Model Higgs boson produced in
association with a top-quark pair, [Formula: see text], is
presented. The analysis uses 20.3 fb<sup>-1</sup> of
<i>pp</i> collision data at [Formula: see text], collected
with the ATLAS detector at the Large Hadron Collider during
2012. The search is designed for the [Formula: see text]
decay mode and uses events containing one or two electrons
or muons. In order to improve the sensitivity of the search,
events are categorised according to their jet and
<i>b</i>-tagged jet multiplicities. A neural network is used
to discriminate between signal and background events, the
latter being dominated by [Formula: see text]+jets
production. In the single-lepton channel, variables
calculated using a matrix element method are included as
inputs to the neural network to improve discrimination of
the irreducible [Formula: see text] background. No
significant excess of events above the background
expectation is found and an observed (expected) limit of 3.4
(2.2) times the Standard Model cross section is obtained at
95 % confidence level. The ratio of the measured [Formula:
see text] signal cross section to the Standard Model
expectation is found to be [Formula: see text] assuming a
Higgs boson mass of 125[Formula: see text].},
Doi = {10.1140/epjc/s10052-015-3543-1},
Key = {fds321303}
}
@article{fds308374,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Connors, J and Convery, ME and Conway,
J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann,
JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Search for the standard model Higgs Boson produced in
association with top quarks using the full CDF data
set.},
Journal = {Physical review letters},
Volume = {109},
Number = {18},
Pages = {181802},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.109.181802},
Abstract = {A search is presented for the standard model Higgs boson
produced in association with top quarks using the full Run
II proton-antiproton collision data set, corresponding to
9.45 fb(-1), collected by the Collider Detector at Fermilab.
No significant excess over the expected background is
observed, and 95% credibility-level upper bounds are placed
on the cross section σ(ttH → lepton + missing transverse
energy+jets). For a Higgs boson mass of 125 GeV/c(2), we
expect to set a limit of 12.6 and observe a limit of 20.5
times the standard model rate. This represents the most
sensitive search for a standard model Higgs boson in this
channel to date.},
Doi = {10.1103/physrevlett.109.181802},
Key = {fds308374}
}
@article{fds308752,
Author = {Collaboration, DAEACDF},
Title = {Search for the Supersymmetric Partner of the Top Quark in
Dilepton Events from pp-bar Collisions at sqrt[s]=1.8
TeV},
Journal = {Physical Review Letters},
Volume = {90},
Number = {25 I},
Pages = {251801},
Year = {2003},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.90.251801},
Abstract = {We have searched for pair production of the supersymmetric
partner of the top quark (stop) in 107 pb-1 of pp-bar
collisions at sqrt[s]=1.8 TeV collected by the Collider
Detector at Fermilab (CDF). Each stop is assumed to decay
into a lepton, bottom quark, and supersymmetric neutrino.
Such a scenario would give rise to events with two leptons,
two hadronic jets, and a substantial imbalance of transverse
energy. No evidence of such a stop signal has been found. We
exclude stop masses in the region (80},
Doi = {10.1103/physrevlett.90.251801},
Key = {fds308752}
}
@article{fds308780,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman,
J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D},
Title = {Search for the supersymmetric partner of the top quark in
pp̄ collisions at √s=1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {63},
Number = {9},
Pages = {911011-911016},
Year = {2001},
Month = {August},
Abstract = {We report on a search for the supersymmetric partner of the
top quark (top squark) produced in tt̄ events using 110
pb-1 of pp̄ collisions at √s = 1.8 TeV recorded with the
Collider Detector at Fermilab. In the case of a light top
squark, the decay of the top quark into a top squark plus
the lightest supersymmetric particle (LSP) could have a
significant branching ratio. The observed events are
consistent with standard model tt̄ production and decay.
Hence, we set limits on the branching ratio of the top quark
decaying into a top squark plus LSP, excluding branching
ratios above 45% for a LSP mass up to 40
GeV/c2.},
Key = {fds308780}
}
@article{fds308917,
Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cen, Y and Cervelli, F and Chapman, J and Cheng,
M},
Title = {Search for the top quark decaying to a charged Higgs boson
in p-barp collisions at sqrt s =1.8 TeV.},
Journal = {Physical review letters},
Volume = {73},
Number = {20},
Pages = {2667-2671},
Publisher = {American Physical Society (APS)},
Year = {1994},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.73.2667},
Abstract = {We present the results of a search in p̄p collisions at
s=1.8 TeV for the top quark decaying to a charged Higgs
boson (H±). We search for dilepton final states from the
decay chain tt̄→HH (or HW, or WW) + bb̄→ll+X. In a
sample of 19.3 pb-1 collected during 1992-93 with the
Collider Detector at Fermilab, we observe 2 events with a
background estimation of 3.0 ± 1.0 events. Limits at 95%
C.L. in the (Mtop,MH±) plane are presented. For the case
Mtop<MW+Mb, we exclude at 95% C.L. the entire (Mtop,MH±)
plane for the branching ratio B(H→τν) larger than 75%.
We also interpret the results in terms of the parameter tan
β of two-Higgs-doublet models. © 1994 The American
Physical Society.},
Doi = {10.1103/physrevlett.73.2667},
Key = {fds308917}
}
@article{fds321275,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for the Xb and other hidden-beauty states
in the π+π−ϒ(1S) channel at
ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {740},
Pages = {199-217},
Publisher = {Elsevier BV},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2014.11.055},
Abstract = {This Letter presents a search for a hidden-beauty
counterpart of the X(3872) in the mass ranges of
10.05–10.31 GeV and 10.40–11.00 GeV, in the channel
Xb→π+π−ϒ(1S)(→μ+μ−), using 16.2 fb−1 of s=8
TeV pp collision data collected by the ATLAS detector at the
LHC. No evidence for new narrow states is found, and upper
limits are set on the product of the Xb cross section and
branching fraction, relative to those of the ϒ(2S), at the
95% confidence level using the CLS approach. These limits
range from 0.8% to 4.0%, depending on mass. For masses above
10.1 GeV, the expected upper limits from this analysis are
the most restrictive to date. Searches for production of the
ϒ(13DJ), ϒ(10860), and ϒ(11020) states also reveal no
significant signals.},
Doi = {10.1016/j.physletb.2014.11.055},
Key = {fds321275}
}
@article{fds376065,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye,
T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja,
S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L},
Title = {Search for the Zγ decay mode of new high-mass resonances in
pp collisions at s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {848},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138394},
Abstract = {This letter presents a search for narrow, high-mass
resonances in the Zγ final state with the Z boson decaying
into a pair of electrons or muons. The s=13 TeV pp collision
data were recorded by the ATLAS detector at the CERN Large
Hadron Collider and have an integrated luminosity of 140
fb−1. The data are found to be in agreement with the
Standard Model background expectation. Upper limits are set
on the resonance production cross section times the decay
branching ratio into Zγ. For spin-0 resonances produced via
gluon–gluon fusion, the observed limits at 95% confidence
level vary between 65.5 fb and 0.6 fb, while for spin-2
resonances produced via gluon–gluon fusion (or
quark–antiquark initial states) limits vary between 77.4
(76.1) fb and 0.6 (0.5) fb, for the mass range from 220 GeV
to 3400 GeV.},
Doi = {10.1016/j.physletb.2023.138394},
Key = {fds376065}
}
@article{fds308463,
Author = {Aaltonen, TEA},
Title = {Search for the {H}iggs boson in the all-hadronic final state
using the {CDF II} detector},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {5},
Pages = {052010},
Publisher = {American Physical Society},
Year = {2011},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.84.052010},
Abstract = {We report on a search for the production of the Higgs boson
decaying to two bottom quarks accompanied by two additional
quarks. The data sample used corresponds to an integrated
luminosity of approximately 4fb-1 of pp̄ collisions at
√s=1.96TeV recorded by the CDF II experiment. This search
includes twice the integrated luminosity of the previous
published result, uses analysis techniques to distinguish
jets originating from light flavor quarks and those from
gluon radiation, and adds sensitivity to a Higgs boson
produced by vector boson fusion. We find no evidence of the
Higgs boson and place limits on the Higgs boson production
cross section for Higgs boson masses between 100GeV/c2 and
150GeV/c2 at the 95% confidence level. For a Higgs boson
mass of 120GeV/c2, the observed (expected) limit is 10.5
(20.0) times the predicted standard model cross section. ©
2011 American Physical Society.},
Doi = {10.1103/PhysRevD.84.052010},
Key = {fds308463}
}
@article{fds308850,
Author = {al, FAE},
Title = {Search for third generation leptoquarks in (p)over-bar-p
collisions at root s=1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {78},
Number = {15},
Pages = {2906-2911},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevLett.78.2906},
Abstract = {We present the results of a search for third generation
leptoquark (LQ) pairs in 110±8pb of p p collisions at
√s=1.8TeV recorded by the Collider Detector at Fermilab.
We assume third generation leptoquarks decay to a Τ lepton
and a bquark with brancing ratio β. We observe one
candidate event, consistent with standard model background
expectations. We place upper limits on σ(p p→LQLQ )β as
a function of the leptoquark mass M . We exclude at 95%
confidence level scalar leptoquarks with M <99GeV/c , gauge
vector leptoquarks with MLQ<225GeV/c , and nongauge vector
leptoquarks with M <170GeV/c for β=1. © 1996 American
Physical Society. ࢤ1 ¯ ¯ ¯ 2 2 2 2 LQ LQ
LQ},
Doi = {10.1103/PhysRevLett.78.2906},
Key = {fds308850}
}
@article{fds308364,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Search for third generation scalar leptoquarks in pp
collisions at √s=7 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {6},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP06(2013)033},
Abstract = {A search for pair-produced third generation scalar
leptoquarks is presented, using proton-proton collisions at
s=7 TeV at the LHC. The data were recorded with the ATLAS
detector and correspond to an integrated luminosity of 4.7
fb-1. Each leptoquark is assumed to decay to a tau lepton
and a b-quark with a branching fraction equal to 100%. No
statistically significant excess above the Standard Model
expectation is observed. Third generation leptoquarks are
therefore excluded at 95% confidence level for masses less
than 534GeV. [Figure not available: see fulltext.] © 2013
Cern for the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP06(2013)033},
Key = {fds308364}
}
@article{fds314172,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Search for top quark decays t → qH with H → γγ using
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {6},
Year = {2014},
Month = {January},
ISSN = {1126-6708},
url = {http://dx.doi.org/10.1007/JHEP06(2014)008},
Abstract = {A search is performed for flavour-changing neutral currents
in the decay of a top quark to an up-type (c, u) quark and a
Higgs boson, where the Higgs boson decays to two photons.
The proton-proton collision data set used corresponds to 4.7
fb-1 at √ = 7TeV and 20.3fb-1 at √ = 8TeV collected by
the ATLAS experiment at the LHC. Top quark pair events are
searched for in which one top quark decays to qH and the
other decays to bW. Both the hadronic and the leptonic decay
modes of the W boson are used. No significant signal is
observed and an upper limit is set on the t → qH branching
ratio of 0.79 at the 95% confidence level. The corresponding
limit on the tqH coupling combination λtcH2 + λtuH2 is
0.17. © 2014 The Author(s).},
Doi = {10.1007/JHEP06(2014)008},
Key = {fds314172}
}
@article{fds321320,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for top squark pair production in final states with
one isolated lepton, jets, and missing transverse momentum
in √ s = 8 TeV pp collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {11},
Publisher = {Springer Nature},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2014)118},
Abstract = {The results of a search for top squark (stop) pair
production in final states with one isolated lepton, jets,
and missing transverse momentum are reported. The analysis
is performed with proton-proton collision data at (Formula
presented.) = 8 TeV collected with the ATLAS detector at the
LHC in 2012 corresponding to an integrated luminosity of 20
fb−1. The lightest supersymmetric particle (LSP) is taken
to be the lightest neutralino which only interacts weakly
and is assumed to be stable. The stop decay modes considered
are those to a top quark and the LSP as well as to a bottom
quark and the lightest chargino, where the chargino decays
to the LSP by emitting a W boson. A wide range of scenarios
with different mass splittings between the stop, the
lightest neutralino and the lightest chargino are
considered, including cases where the W bosons or the top
quarks are off-shell. Decay modes involving the heavier
charginos and neutralinos are addressed using a set of
phenomenological models of supersymmetry. No significant
excess over the Standard Model prediction is observed. A
stop with a mass between 210 and 640 GeV decaying directly
to a top quark and a massless LSP is excluded at 95%
confidence level, and in models where the mass of the
lightest chargino is twice that of the LSP, stops are
excluded at 95% confidence level up to a mass of 500 GeV for
an LSP mass in the range of 100 to 150 GeV. Stringent
exclusion limits are also derived for all other stop decay
modes considered, and model-independent upper limits are set
on the visible cross-section for processes beyond the
Standard Model.},
Doi = {10.1007/JHEP11(2014)118},
Key = {fds321320}
}
@article{fds365422,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA},
Title = {Search for top squarks in events with a Higgs or Z boson
using 139 fb - 1 of pp collision data at √s=13
TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {11},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08469-8},
Abstract = {This paper presents a search for direct top squark pair
production in events with missing transverse momentum plus
either a pair of jets consistent with Standard Model Higgs
boson decay into b-quarks or a same-flavour opposite-sign
dilepton pair with an invariant mass consistent with a Z
boson. The analysis is performed using the proton–proton
collision data at s=13 TeV collected with the ATLAS detector
during the LHC Run-2, corresponding to an integrated
luminosity of 139 fb- 1. No excess is observed in the data
above the Standard Model predictions. The results are
interpreted in simplified models featuring direct production
of pairs of either the lighter top squark (t~ 1) or the
heavier top squark (t~ 2), excluding at 95% confidence level
t~ 1 and t~ 2 masses up to about 1220 and 875 GeV,
respectively.},
Doi = {10.1140/epjc/s10052-020-08469-8},
Key = {fds365422}
}
@article{fds321171,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for top squarks in final states with one isolated
lepton, jets, and missing transverse momentum in s =13 TeV
pp collisions with the ATLAS detector},
Journal = {Physical Review D},
Volume = {94},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.94.052009},
Abstract = {The results of a search for the top squark, the
supersymmetric partner of the top quark, in final states
with one isolated electron or muon, jets, and missing
transverse momentum are reported. The search uses the 2015
LHC pp collision data at a center-of-mass energy of s=13 TeV
recorded by the ATLAS detector and corresponding to an
integrated luminosity of 3.2 fb-1. The analysis targets two
types of signal models: gluino-mediated pair production of
top squarks with a nearly mass-degenerate top squark and
neutralino and direct pair production of top squarks,
decaying to the top quark and the lightest neutralino. The
experimental signature in both signal scenarios is similar
to that of a top quark pair produced in association with
large missing transverse momentum. No significant excess
over the Standard Model background prediction is observed,
and exclusion limits on gluino and top squark masses are set
at 95% confidence level. The results extend the LHC run-1
exclusion limit on the gluino mass up to 1460 GeV in the
gluino-mediated scenario in the high gluino and low top
squark mass region and add an excluded top squark mass
region from 745 to 780 GeV for the direct top squark model
with a massless lightest neutralino. The results are also
reinterpreted to set exclusion limits in a model of
vectorlike top quarks.},
Doi = {10.1103/PhysRevD.94.052009},
Key = {fds321171}
}
@article{fds308529,
Author = {Aaltonen, T and others},
Title = {Search for Top-Quark Production via Flavor-Changing Neutral
Currents in W + 1 Jet Events at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {15},
Pages = {151801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.151801},
Abstract = {We report on a search for the non-standard-model process
u(c) + g --> t using pp[over ] collision data collected by
the Collider Detector at Fermilab II detector corresponding
to 2.2 fb;{-1}. The candidate events are classified as
signal-like or backgroundlike by an artificial neural
network. The observed discriminant distribution yields no
evidence for flavor-changing neutral current top-quark
production, resulting in an upper limit on the production
cross section sigma(u(c) + g --> t) < 1.8 pb at the 95% C.L.
Using theoretical predictions we convert the cross section
limit to upper limits on flavor-changing neutral current
branching ratios: B(t --> u + g) < 3.9 x 10;{-4} and B(t -->
c + g) < 5.7 x 10;{-3}.},
Doi = {10.1103/physrevlett.102.151801},
Key = {fds308529}
}
@article{fds335597,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for top-squark pair production in final states with
one lepton, jets, and missing transverse momentum using 36
fb−1 of √s=13 TeV pp collision data with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {6},
Publisher = {Springer Nature},
Year = {2018},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2018)108},
Abstract = {The results of a search for the direct pair production of
top squarks, the supersymmetric partner of the top quark, in
final states with one isolated electron or muon, several
energetic jets, and missing transverse momentum are
reported. The analysis also targets spin-0 mediator models,
where the mediator decays into a pair of dark-matter
particles and is produced in association with a pair of top
quarks. The search uses data from proton-proton collisions
delivered by the Large Hadron Collider in 2015 and 2016 at a
centre-of-mass energy of s=13 TeV and recorded by the ATLAS
detector, corresponding to an integrated luminosity of 36
fb−1. A wide range of signal scenarios with different
mass-splittings between the top squark, the lightest
neutralino and possible intermediate supersymmetric
particles are considered, including cases where the W bosons
or the top quarks produced in the decay chain are off-shell.
No significant excess over the Standard Model prediction is
observed. The null results are used to set exclusion limits
at 95% confidence level in several supersymmetry benchmark
models. For pair-produced top-squarks decaying into top
quarks, top-squark masses up to 940 GeV are excluded.
Stringent exclusion limits are also derived for all other
considered top-squark decay scenarios. For the spin-0
mediator models, upper limits are set on the visible
cross-section.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP06(2018)108},
Key = {fds335597}
}
@article{fds365425,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
Title = {Search for tt¯ resonances in fully hadronic final states in
pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2020)061},
Abstract = {This paper presents a search for new heavy particles
decaying into a pair of top quarks using 139 fb−1 of
proton-proton collision data recorded at a centre-of-mass
energy of s = 13 TeV with the ATLAS detector at the Large
Hadron Collider. The search is performed using events
consistent with pair production of high-transverse-momentum
top quarks and their subsequent decays into the fully
hadronic final states. The analysis is optimized for
resonances decaying into a tt¯ pair with mass above 1.4
TeV, exploiting a dedicated multivariate technique with jet
substructure to identify hadronically decaying top quarks
using large-radius jets and evaluating the background
expectation from data. No significant deviation from the
background prediction is observed. Limits are set on the
production cross-section times branching fraction for the
new Z′ boson in a topcolor-assisted-technicolor model. The
Z′ boson masses below 3.9 and 4.7 TeV are excluded at 95%
confidence level for the decay widths of 1% and 3%,
respectively. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP10(2020)061},
Key = {fds365425}
}
@article{fds308322,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
Title = {Search for tt̄ resonances in the lepton plus jets final
state with ATLAS using 4.7 fb–1of pp collisions
at √s = 7 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.88.012004},
Abstract = {A search for new particles that decay into top quark pairs
(tt) is performed with the ATLAS experiment at the LHC using
an integrated luminosity of 4.7 fb–1of proton–proton
(pp) collision data collected at a center-of-mass energy
√s = 7 TeV. In the tt̄→ WbWb decay, the lepton plus
jets final state is used, where one W boson decays
leptonically and the other hadronically. The tt̄system is
reconstructed using both small-radius and large-radius jets,
the latter being supplemented by a jet substructure
analysis. A search for local excesses in the number of data
events compared to the Standard Model expectation in the
tt̄invariant mass spectrum is performed. No evidence for a
tt̄resonance is found and 95% credibility-level limits on
the production rate are determined for massive states
predicted in two benchmark models. The upper limits on the
cross section times branching ratio of a narrow Z′
resonance range from 5.1 pb for a boson mass of 0.5 TeV to
0.03 pb for a mass of 3 TeV. A narrow leptophobic topcolor
Z′ resonance with a mass below 1.74 TeV is excluded.
Limits are also derived for a broad color-octet resonance
with Γ/m = 15.3%. A Kaluza–Klein excitation of the gluon
in a Randall–Sundrum model is excluded for masses below
2.07 TeV.},
Doi = {10.1103/PhysRevD.88.012004},
Key = {fds308322}
}
@article{fds365408,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Search for type-III seesaw heavy leptons in dilepton final
states in pp collisions at √s=13TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {3},
Year = {2021},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-08929-9},
Abstract = {A search for the pair production of heavy leptons as
predicted by the type-III seesaw mechanism is presented. The
search uses proton–proton collision data at a
centre-of-mass energy of 13 TeV, corresponding to 139fb-1
of integrated luminosity recorded by the ATLAS detector
during Run 2 of the Large Hadron Collider. The analysis
focuses on the final state with two light leptons (electrons
or muons) of different flavour and charge combinations, with
at least two jets and large missing transverse momentum. No
significant excess over the Standard Model expectation is
observed. The results are translated into exclusion limits
on heavy-lepton masses, and the observed lower limit on the
mass of the type-III seesaw heavy leptons is 790 GeV at 95%
confidence level.},
Doi = {10.1140/epjc/s10052-021-08929-9},
Key = {fds365408}
}
@article{fds367720,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alconada
Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Search for type-III seesaw heavy leptons in leptonic final
states in pp collisions at √s=13TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {11},
Year = {2022},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10785-0},
Abstract = {A search for the pair production of heavy leptons as
predicted by the type-III seesaw mechanism is presented. The
search uses proton–proton collision data at a
centre-of-mass energy of 13 TeV, corresponding to 139fb-1
of integrated luminosity recorded by the ATLAS detector
during Run 2 of the Large Hadron Collider. The analysis
focuses on final states with three or four electrons or
muons from the possible decays of new heavy leptons via
intermediate electroweak bosons. No significant deviations
above the Standard Model expectation are observed; upper and
lower limits on the heavy lepton production cross-section
and masses are derived respectively. These results are then
combined for the first time with the ones already published
by ATLAS using the channel with two leptons in the final
state. The observed lower limit on the mass of the type-III
seesaw heavy leptons combining two, three and four lepton
channels together is 910 GeV at the 95% confidence
level.},
Doi = {10.1140/epjc/s10052-022-10785-0},
Key = {fds367720}
}
@article{fds321232,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for type-III seesaw heavy leptons in pp collisions at
s =8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.92.032001},
Abstract = {A search for the pair production of heavy leptons (N0,L±)
predicted by the type-III seesaw theory formulated to
explain the origin of small neutrino masses is presented.
The decay channels N0→W±l (=e,μ,τ) and L±→W±ν
(ν=νe,νμ,ντ) are considered. The analysis is performed
using the final state that contains two leptons (electrons
or muons), two jets from a hadronically decaying W boson and
large missing transverse momentum. The data used in the
measurement correspond to an integrated luminosity of 20.3
fb-1 of pp collisions at s=8 TeV collected by the ATLAS
detector at the LHC. No evidence of heavy lepton pair
production is observed. Heavy leptons with masses below
325-540 GeV are excluded at the 95% confidence level,
depending on the theoretical scenario considered.},
Doi = {10.1103/PhysRevD.92.032001},
Key = {fds321232}
}
@article{fds308633,
Author = {Abulencia, and A, and others},
Title = {Search for V + A current in top quark decay in p anti-p
collisions at s**(1/2) = 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {7},
Pages = {072001},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.072001},
Abstract = {We report an upper limit on the fraction of V+A current,
fV+A, in top-quark decays, using approximately 700 pb-1 of
p[overline p] collisions at sqrt(s)=1.96 TeV acquired by the
upgraded Collider Detector at Fermilab. For the decay
t-->Wb-->[script-l]nub (where [script-l]=e or µ), the
invariant mass of the charged lepton and the bottom quark
jet is sensitive to the polarization of the W boson. We
determine fV+A=-0.06$\pm$0.25 given a top-quark mass of 175
GeV/c2. We set an upper limit on fV+A of 0.29 at the 95\%
confidence level, an improvement by a factor of 2 on the
previous best direct limit.},
Doi = {10.1103/physrevlett.98.072001},
Key = {fds308633}
}
@article{fds321247,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G},
Title = {Search for vectorlike B quarks in events with one isolated
lepton, missing transverse momentum, and jets at s =8 TeV
with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.91.112011},
Abstract = {A search has been performed for pair production of heavy
vectorlike down-type (B) quarks. The analysis explores the
lepton-plus-jets final state, characterized by events with
one isolated charged lepton (electron or muon), significant
missing transverse momentum, and multiple jets. One or more
jets are required to be tagged as arising from b quarks, and
at least one pair of jets must be tagged as arising from the
hadronic decay of an electroweak boson. The analysis uses
the full data sample of pp collisions recorded in 2012 by
the ATLAS detector at the LHC, operating at a center-of-mass
energy of 8 TeV, corresponding to an integrated luminosity
of 20.3 fb-1. No significant excess of events is observed
above the expected background. Limits are set on vectorlike
B production, as a function of the B branching ratios,
assuming the allowable decay modes are B→Wt/Zb/Hb. In the
chiral limit with a branching ratio of 100% for the decay
B→Wt, the observed (expected) 95% C.L. lower limit on the
vectorlike B mass is 810 GeV (760 GeV). In the case where
the vectorlike B quark has branching ratio values
corresponding to those of an SU(2) singlet state, the
observed (expected) 95% C.L. lower limit on the vectorlike B
mass is 640 GeV (505 GeV). The same analysis, when used to
investigate pair production of a colored, charge 5/3 exotic
fermion T5/3, with subsequent decay T5/3→Wt, sets an
observed (expected) 95% C.L. lower limit on the T5/3 mass of
840 GeV (780 GeV).},
Doi = {10.1103/PhysRevD.91.112011},
Key = {fds321247}
}
@article{fds308700,
Author = {Brozovic, M and Goshaw, A and Kruse, M and U, WRD and Collaboration,
WDAEACDF},
Title = {Search for W and Z bosons in $p\bar{p} \to 2\ {\rm jets} +
\gamma$ at $sqrt{s} = 1.8$ TeV},
Journal = {Phys. Rev. D},
Volume = {73},
Number = {012001},
Year = {2006},
url = {http://arxiv.org/pdf/hep-ex/0507051},
Abstract = {We present a study of the dijet invariant mass distribution
for the reaction p̄p→twojets+γ+X, at a center of mass
energy of 1.8 TeV, using data collected by the CDF
experiment. We compare the data to predictions for the
production of a photon with two jets, together with the
resonant processes p̄p→W/Z+γ+X, in which the W and Z
bosons decay hadronically. A fit is made to the dijet
invariant mass distribution combining the nonresonant
background and resonant processes. We use the result to
establish a limit for the inclusive production cross section
of W/Z+γ with hadronic decay of the W and Z bosons. © 2006
The American Physical Society.},
Doi = {10.1103/PhysRevD.73.012001},
Key = {fds308700}
}
@article{fds335601,
Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brozovic, M and Brubaker, E and Budagov,
J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu,
ML and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R and Dagenhart, D and D'Auria, S and de
Barbaro, P and de Cecco, S and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and de Pedis, D and Derwent,
PF and Dionisi, C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede,
D},
Title = {Search for W and Z bosons in the reaction p̄p→twojets+γ
at s=1.8TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {73},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2006},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.73.012001},
Abstract = {We present a study of the dijet invariant mass distribution
for the reaction p̄p→twojets+γ+X, at a center of mass
energy of 1.8 TeV, using data collected by the CDF
experiment. We compare the data to predictions for the
production of a photon with two jets, together with the
resonant processes p̄p→W/Z+γ+X, in which the W and Z
bosons decay hadronically. A fit is made to the dijet
invariant mass distribution combining the nonresonant
background and resonant processes. We use the result to
establish a limit for the inclusive production cross section
of W/Z+γ with hadronic decay of the W and Z bosons. © 2006
The American Physical Society.},
Doi = {10.1103/PhysRevD.73.012001},
Key = {fds335601}
}
@article{fds321277,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
Title = {Search for W ′ → t b ¯ in the lepton plus jets final
state in proton–proton collisions at a centre-of-mass
energy of s = 8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {743},
Pages = {235-255},
Publisher = {Elsevier BV},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2015.02.051},
Abstract = {A search for new charged massive gauge bosons, called W′,
is performed with the ATLAS detector at the LHC, in
proton–proton collisions at a centre-of-mass energy of s=8
TeV, using a dataset corresponding to an integrated
luminosity of 20.3 fb−1. This analysis searches for W′
bosons in the W′→tb¯ decay channel in final states with
electrons or muons, using a multivariate method based on
boosted decision trees. The search covers masses between 0.5
and 3.0 TeV, for right-handed or left-handed W′ bosons. No
significant deviation from the Standard Model expectation is
observed and limits are set on the W′→tb¯ cross-section
times branching ratio and on the W′-boson effective
couplings as a function of the W′-boson mass using the CLs
procedure. For a left-handed (right-handed) W′ boson,
masses below 1.70 (1.92) TeV are excluded at 95% confidence
level.},
Doi = {10.1016/j.physletb.2015.02.051},
Key = {fds321277}
}
@article{fds308649,
Author = {Abulencia, and A, and others},
Title = {Search for W' boson decaying to electron-neutrino pairs in p
anti-p collisions at s**(1/2) = 1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {9},
Pages = {091101},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.091101},
Abstract = {We present the results of a search for W[prime] boson
decaying to electron-neutrino pairs in p[overline p]
collisions at a center-of-mass energy of 1.96 TeV, using a
data sample corresponding to 205 pb-1 of integrated
luminosity collected by the CDF II detector at Fermilab. We
observe no evidence for this decay mode and set limits on
the production cross section times branching fraction,
assuming the neutrinos from W[prime] boson decays to be
light. If we assume the manifest left-right symmetric model,
we exclude a W[prime] boson with mass less than 788 GeV/c2
at the 95\% confidence level.},
Doi = {10.1103/PhysRevD.75.091101},
Key = {fds308649}
}
@article{fds308335,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Search for WH production with a light Higgs boson decaying
to prompt electron-jets in proton-proton collisions at
√s=7 TeV with the ATLAS detector},
Journal = {New Journal of Physics},
Volume = {15},
Number = {4},
Pages = {043009-043009},
Publisher = {IOP Publishing},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1088/1367-2630/15/4/043009},
Abstract = {A search is performed for WH production with a light Higgs
boson decaying to hidden-sector particles resulting in
clusters of collimated electrons, known as electron-jets.
The search is performed with 2.04 fb-1 of data collected in
2011 with the ATLAS detector at the Large Hadron Collider in
proton-proton collisions at . One event satisfying the
signal selection criteria is observed, which is consistent
with the expected background rate. Limits on the product of
the WH production cross section and the branching ratio of a
Higgs boson decaying to prompt electron-jets are calculated
as a function of a Higgs boson mass in the range from 100 to
140 GeV. © CERN 2013 for the benefit of the ATLAS
Collaboration, published under the terms of the Creative
Commons Attribution 3.0 licence by IOP Publishing Ltd and
Deutsche Physikalische Gesellschaft. Any further
distribution of this work must maintain attribution to the
author(s) and the published article's title, journal
citation and DOI.},
Doi = {10.1088/1367-2630/15/4/043009},
Key = {fds308335}
}
@article{fds308567,
Author = {Aaltonen, T and others},
Title = {Search for WW and WZ production in lepton plus jets final
state at CDF},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {11},
Pages = {112011},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.112011},
Abstract = {We present a search for WW and WZ production in final states
that contain a charged lepton (electron or muon) and at
least two jets, produced in sqrt[s]=1.96 TeV pp̅
collisions at the Fermilab Tevatron, using data
corresponding to 1.2 fb-1 of integrated luminosity
collected with the CDF II detector. Diboson production in
this decay channel has yet to be observed at hadron
colliders due to the large single W plus jets background. An
artificial neural network has been developed to increase
signal sensitivity, as compared with an event selection
based on conventional cuts. We set a 95% confidence level
upper limit of σWW×BR(W→ℓνℓ,W→jets)+σWZ×BR(W→ℓνℓ,Z→jets)<2.88 pb,
which is consistent with the standard model
next-to-leading-order cross section calculation for this
decay channel of 2.09 ± 0.12 pb.},
Doi = {10.1103/PhysRevD.79.112011},
Key = {fds308567}
}
@article{fds321322,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for WZ resonances in the fully leptonic channel using
pp collisions at s=8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {737},
Pages = {223-243},
Publisher = {Elsevier BV},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2014.08.039},
Abstract = {A search for resonant WZ production in the ℓνℓ'ℓ'
(ℓ,ℓ'=e,μ) decay channel using 20.3 fb-1 of s=8TeV pp
collision data collected by the ATLAS experiment at LHC is
presented. No significant deviation from the Standard Model
prediction is observed and upper limits on the production
cross sections of WZ resonances from an extended gauge model
W' and from a simplified model of heavy vector triplets are
derived. A corresponding observed (expected) lower mass
limit of 1.52 (1.49) TeV is derived for the W' at the 95%
confidence level. © 2014 Elsevier B.V.},
Doi = {10.1016/j.physletb.2014.08.039},
Key = {fds321322}
}
@article{fds308403,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca almenar, C and Cuevas, J and Culbertson, R and Dagenhart, D},
Title = {Search for WZ+ZZ production with missing transverse
energy+jets with b enhancement at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012002},
Abstract = {Diboson production (WW+WZ+ZZ) has been observed at the
Tevatron in hadronic decay modes dominated by the WW
process. This paper describes the measurement of the cross
section of WZ and ZZ events in final states with large E T
and using b-jet identification as a tool to suppress WW
contributions. Because of the limited energy resolution, we
cannot distinguish between partially hadronic decays of WZ
and ZZ, and we measure the sum of these processes. The
number of signal events is extracted using a simultaneous
fit to the invariant mass distribution of the two jets for
events with two b-jet candidates and events with fewer than
two b-jet candidates. We measure a cross section
σ(pp̄→WZ,ZZ)=5.8-3.0+3.6pb, in agreement with the
standard model. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.85.012002},
Key = {fds308403}
}
@article{fds308729,
Author = {Cabrera, S and Carron, S and Goshaw, A and Hays, C and Huang, Y and U, MKD and Collaboration, WDAEACDF},
Title = {Search for ZZ and ZW Production in ppbar Collisions at
$\sqrt{s} = 1.96$ TeV},
Journal = {Phys. Rev. D},
Volume = {71},
Number = {091105},
Year = {2005},
url = {http://arxiv.org/pdf/hep-ex/0501021},
Abstract = {http://arxiv.org/abs/hep-ex/0501021},
Key = {fds308729}
}
@article{fds335602,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
AG and Clark, D and Coca, M and Connolly, A},
Title = {Search for ZZ and ZW production in pp̄ collisions at
s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {9},
Pages = {1-7},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.71.091105},
Abstract = {We present a search for ZZ and ZW vector boson pair
production in pp̄ collisions at s=1.96TeV using the
leptonic decay channels ZZ→llνν, ZZ→lll′l′, and
ZW→lll′ν. In a data sample corresponding to an
integrated luminosity of 194pb-1 collected with the Collider
Detector at Fermilab, 3 candidate events are found with an
expected background of 1.0±0.2 events. We set a 95%
confidence level upper limit of 15.2pb on the cross section
for ZZ plus ZW production, compared to the standard model
prediction of 5.0±0.4pb. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevD.71.091105},
Key = {fds335602}
}
@article{fds321291,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Search for [Formula: see text] decays in [Formula: see text]
collisions at [Formula: see text] = 8 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {4},
Pages = {165},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3372-2},
Abstract = {A search for a massive [Formula: see text] gauge boson
decaying to a top quark and a bottom quark is performed with
the ATLAS detector in [Formula: see text] collisions at the
LHC. The dataset was taken at a centre-of-mass energy of
[Formula: see text] and corresponds to [Formula: see text]
of integrated luminosity. This analysis is done in the
hadronic decay mode of the top quark, where novel jet
substructure techniques are used to identify jets from
high-momentum top quarks. This allows for a search for
high-mass [Formula: see text] bosons in the range
1.5-3.0 [Formula: see text]. [Formula: see text]-tagging is
used to identify jets originating from [Formula: see
text]-quarks. The data are consistent with Standard Model
background-only expectations, and upper limits at 95 %
confidence level are set on the [Formula: see text] cross
section times branching ratio ranging from [Formula: see
text] to [Formula: see text] for left-handed [Formula: see
text] bosons, and ranging from [Formula: see text] to
[Formula: see text] for [Formula: see text] bosons with
purely right-handed couplings. Upper limits at 95 %
confidence level are set on the [Formula: see text]-boson
coupling to [Formula: see text] as a function of the
[Formula: see text] mass using an effective field theory
approach, which is independent of details of particular
models predicting a [Formula: see text] boson.},
Doi = {10.1140/epjc/s10052-015-3372-2},
Key = {fds321291}
}
@article{fds308456,
Author = {Aaltonen, and T, and al, E},
Title = {Search for {Randall-Sundrum} gravitons in the diphoton
channel at {CDF}},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {1},
Pages = {011102},
Publisher = {American Physical Society},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.83.011102},
Abstract = {We report on a search for new particles in the diphoton
channel using a data sample of pp̄ collisions at
√s=1.96TeV collected by the CDF II detector at the
Fermilab Tevatron, with an integrated luminosity of
5.4fb⊃-1. The diphoton invariant mass spectrum of the data
agrees well with the standard model expectation. We set
upper limits on the production cross section times branching
ratio for the Randall-Sundrum graviton, as a function of
diphoton mass. We subsequently derive lower limits on the
graviton mass of 459GeV/c2 and 963GeV/c2, at the 95%
confidence level, for coupling parameters (k/M̄Pl) of 0.01
and 0.1, respectively. © 2011 American Physical
Society.},
Doi = {10.1103/PhysRevD.83.011102},
Key = {fds308456}
}
@article{fds375937,
Author = {Amerl, M and Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi,
G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori,
G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang,
R and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Ghosh, A and Johns,
KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK},
Title = {Search in diphoton and dielectron final states for displaced
production of Higgs or Z bosons with the ATLAS detector in
Formula Presented pp collisions},
Journal = {Physical Review D},
Volume = {108},
Number = {1},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.108.012012},
Abstract = {A search is presented for displaced production of Higgs
bosons or Z bosons, originating from the decay of a neutral
long-lived particle (LLP) and reconstructed in the decay
modes H → γ γ and Z → e e . The analysis uses the full
Run 2 dataset of proton-proton collisions delivered by the
LHC at an energy of s = 13 TeV between 2015 and 2018 and
recorded by the ATLAS detector, corresponding to an
integrated luminosity of 139 fb - 1 . Exploiting the
capabilities of the ATLAS liquid argon calorimeter to
precisely measure the arrival times and trajectories of
electromagnetic objects, the analysis searches for the
signature of pairs of photons or electrons which arise from
a common displaced vertex and which arrive after some delay
at the calorimeter. The results are interpreted in a
gauge-mediated supersymmetry breaking model with
pair-produced Higgsinos that decay to LLPs, and each LLP
subsequently decays into either a Higgs boson or a Z boson.
The final state includes at least two particles that escape
direct detection, giving rise to missing transverse
momentum. No significant excess is observed above the
background expectation. The results are used to set upper
limits on the cross section for Higgsino pair production, up
to a χ ˜ 1 0 mass of 369 (704) GeV for decays with 100%
branching ratio of χ ˜ 1 0 to Higgs ( Z ) bosons for a χ
˜ 1 0 lifetime of 2 ns. A model-independent limit is also
set on the production of pairs of photons or electrons with
a significant delay in arrival at the calorimeter.},
Doi = {10.1103/PhysRevD.108.012012},
Key = {fds375937}
}
@article{fds308636,
Author = {Aaltonen, T and others},
Title = {Searches for direct pair production of supersymmetric top
and supersymmetric bottom quarks in p[overline p] collisions
at $\sqrt{s}$=1.96 TeV},
Journal = {Phys. Rev.},
Volume = {D76},
Number = {7},
Pages = {072010},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.76.072010},
Abstract = {We search for direct pair production of supersymmetric top
quarks and supersymmetric bottom quarks in proton-antiproton
collisions at sqrt(s)=1.96 TeV, using 295 pb-1 of data
recorded by the Collider Detector at Fermilab (CDF II)
experiment. The supersymmetric top (supersymmetric bottom)
quarks are selected by reconstructing their decay into a
charm (bottom) quark and a neutralino, which is assumed to
be the lightest supersymmetric particle. The signature of
such processes is two energetic heavy-flavor jets and
missing transverse energy. The number of events that pass
our selection for each search process is consistent with the
expected standard model background. By comparing our results
to the theoretical production cross sections of the
supersymmetric top and supersymmetric bottom quarks in the
minimal supersymmetric standard model, we exclude, at a 95%
confidence level in the frame of that model, a
supersymmetric top quark mass up to 132 GeV/c2 for a
neutralino mass of 48 GeV/c2, and a supersymmetric bottom
quark mass up to 193 GeV/c2 for a neutralino mass of 40
GeV/c2.},
Doi = {10.1103/PhysRevD.76.072010},
Key = {fds308636}
}
@article{fds375906,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames,
CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche,
CS and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Searches for exclusive Higgs and Z boson decays into a
vector quarkonium state and a photon using 139 fb -
1 of ATLAS √s=13 TeV proton–proton collision
data},
Journal = {European Physical Journal C},
Volume = {83},
Number = {9},
Year = {2023},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11869-1},
Abstract = {Searches for the exclusive decays of Higgs and Z bosons into
a vector quarkonium state and a photon are performed in the
μ+μ-γ final state with a proton–proton collision data
sample corresponding to an integrated luminosity of 139 fb
- 1 collected at s=13 TeV with the ATLAS detector at the
CERN Large Hadron Collider. The observed data are compatible
with the expected backgrounds. The 95% confidence-level
upper limits on the branching fractions of the Higgs boson
decays into J/ψγ , ψ(2S)γ , and Υ(1S,2S,3S)γ are found
to be 2.0 × 10 - 4 , 10.5 × 10 - 4 , and (2.5 , 4.2 , 3.4)
× 10 - 4 , respectively, assuming Standard Model production
of the Higgs boson. The corresponding 95% CL upper limits on
the branching fractions of the Z boson decays are 1.2 × 10
- 6 , 2.4 × 10 - 6 , and (1.1 , 1.3 , 2.4) × 10 - 6 . An
observed 95% CL interval of (- 133 , 175) is obtained for
the κc/ κγ ratio of Higgs boson coupling modifiers, and a
95% CL interval of (- 37 , 40) is obtained for κb/ κγ
.},
Doi = {10.1140/epjc/s10052-023-11869-1},
Key = {fds375906}
}
@article{fds321169,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Searches for heavy diboson resonances in pp collisions at
√s=13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {9},
Publisher = {Springer Nature},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2016)173},
Abstract = {Searches for new heavy resonances decaying to WW, WZ, and ZZ
bosons are presented, using a data sample corresponding to
3.2 fb−1 of pp collisions at s=13 TeV collected with the
ATLAS detector at the CERN Large Hadron Collider. Analyses
selecting ννqq, ℓνqq, ℓℓqq and qqqq final states
are combined, searching for an arrow-width resonance with
mass between 500 and 3000 GeV. The discriminating variable
is either an invariant mass or a transverse mass. No
significant deviations from the Standard Model predictions
are observed. Three benchmark models are tested: a model
predicting the existence of a new heavy scalar singlet, a
simplified model predicting a heavy vector-boson triplet,
and a bulk Randall-Sundrum model with a heavy spin-2
graviton. Cross-section limits are set at the 95% confidence
level and are compared to theoretical cross-section
predictions for a variety of models. The data exclude a
scalar singlet with mass below 2650 GeV, a heavy
vector-boson triplet with mass below 2600 GeV, and a
graviton with mass below 1100 GeV. These results
significantly extend the previous limits set using pp
collisions at s=8 TeV.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP09(2016)173},
Key = {fds321169}
}
@article{fds321283,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Searches for heavy long-lived charged particles with the
ATLAS detector in proton-proton collisions at √s = 8
Tev},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {1},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2015)068},
Abstract = {Abstract: Searches for heavy long-lived charged particles
are performed using a data sample of 19.1 fb−1 from
proton-proton collisions at a centre-of-mass energy of s=8$$
\sqrt{s}=8 $$ TeV collected by the ATLAS detector at the
Large Hadron Collider. No excess is observed above the
estimated background and limits are placed on the mass of
long-lived particles in various supersymmetric models.
Long-lived tau sleptons in models with gauge-mediated
symmetry breaking are excluded up to masses between 440 and
385 GeV for tan β between 10 and 50, with a 290 GeV limit
in the case where only direct tau slepton production is
considered. In the context of simplified LeptoSUSY models,
where sleptons are stable and have a mass of 300 GeV, squark
and gluino masses are excluded up to a mass of 1500 and 1360
GeV, respectively. Directly produced charginos, in
simplified models where they are nearly degenerate to the
lightest neutralino, are excluded up to a mass of 620 GeV.
R-hadrons, composites containing a gluino, bottom squark or
top squark, are excluded up to a mass of 1270, 845 and 900
GeV, respectively, using the full detector; and up to a mass
of 1260, 835 and 870 GeV using an approach disregarding
information from the muon spectrometer.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP01(2015)068},
Key = {fds321283}
}
@article{fds375945,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
ATH},
Title = {Searches for new phenomena in events with two leptons, jets,
and missing transverse momentum in 139 fb - 1 of
√s=13 TeV pp collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11434-w},
Abstract = {Searches for new phenomena inspired by supersymmetry in
final states containing an e+e- or μ+μ- pair, jets, and
missing transverse momentum are presented. These searches
make use of proton–proton collision data with an
integrated luminosity of 139fb-1 , collected during
2015–2018 at a centre-of-mass energy s=13 TeV by the ATLAS
detector at the Large Hadron Collider. Two searches target
the pair production of charginos and neutralinos. One uses
the recursive-jigsaw reconstruction technique to follow up
on excesses observed in 36.1fb-1 of data, and the other uses
conventional event variables. The third search targets pair
production of coloured supersymmetric particles (squarks or
gluinos) decaying through the next-to-lightest neutralino
(χ~20) via a slepton (ℓ~) or Z boson into ℓ+ℓ-χ~10 ,
resulting in a kinematic endpoint or peak in the dilepton
invariant mass spectrum. The data are found to be consistent
with the Standard Model expectations. Results are
interpreted using simplified models and exclude masses up to
900 GeV for electroweakinos, 1550 GeV for squarks, and
2250 GeV for gluinos.},
Doi = {10.1140/epjc/s10052-023-11434-w},
Key = {fds375945}
}
@article{fds308838,
Author = {Collaboration, CDF},
Title = {Searches for New Physics in Diphoton Events in pp at „©s
= 1.8 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {81},
Number = {9},
Pages = {1791},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.1791},
Abstract = {We have searched for anomalous production of missing ET(ET),
jets, leptons (e, μ, τ), bquarks, or additional photons in
events containing two isolated, central (|η| < 1.0) photons
with ET > 12GeV. The results are consistent with standard
model expectations, with the possible exception of one event
that has in addition to the two photons a central electron,
a high-ET electromagnetic cluster, and large ET. We set
limits using two specific supersymmetry scenarios for
production of diphoton events with ET. © 1998 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.81.1791},
Key = {fds308838}
}
@article{fds308808,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbara, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bikhari, W and Bolla,
G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Burner, N and Brunetti, R and Buckley-Geer, E and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir,
S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch,
H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel,
O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti,
G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn,
SR and Hamilton, R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hausser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman,
KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman,
BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins,
D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch,
L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo,
K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald,
W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone,
S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson,
C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Volobouev, I and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund,
AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu,
X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Searches for new physics in diphoton events in pp̄
collisions at √s = 1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {59},
Number = {9},
Pages = {1-29},
Year = {1999},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.59.092002},
Abstract = {We present a detailed description of a search for anomalous
production of missing ET (Slashed E signT), jets, leptons
(e, μ, τ), b quarks, or additional photons in events
containing two isolated, central (|η|<1.0) photons with
ET>12 GeV. The results are consistent with standard model
expectations, with the possible exception of one event that
has, in addition to the two photons, a central electron, a
high-ET electromagnetic cluster, and large Slashed E signT.
We set limits using two specific SUSY scenarios for
production of diphoton events with Slashed E signT. ©1999
The American Physical Society.},
Doi = {10.1103/PhysRevD.59.092002},
Key = {fds308808}
}
@article{fds330934,
Author = {al, TAE},
Title = {Searches for new physics in events with a photon and b-quark
jet at CDF},
Journal = {Physical Review},
Volume = {D65},
Number = {5},
Pages = {052006},
Publisher = {American Physical Society (APS)},
Year = {2002},
url = {http://dx.doi.org/10.1103/PhysRevD.65.052006},
Abstract = {We have searched for evidence of physics beyond the standard
model in events that include an energetic photon and an
energetic b-quark jet, produced in 85 pb-1 of (image found)
collisions at 1.8 TeV at the Tevatron Collider at Fermilab.
This signature, containing at least one gauge boson and a
third-generation quark, could arise in the production and
decay of a pair of new particles, such as those predicted by
supersymmetry, leading to a production rate exceeding
standard model predictions. We also search these events for
anomalous production of missing transverse energy,
additional jets and leptons (e, µ and τ), and additional b
quarks. We find no evidence for any anomalous production of
γb or γb+X events. We present limits on two supersymmetric
models: a model where the photon is produced in the decay
(equation found), and a model where the photon is produced
in the neutralino decay into the gravitino LSP, (equation
found). We also present our limits in a model-independent
form and test methods of applying model-independent
limits.},
Doi = {10.1103/PhysRevD.65.052006},
Key = {fds330934}
}
@article{fds321205,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and CabreraUrbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace,
N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP},
Title = {Searches for scalar leptoquarks in pp collisions at
[Formula: see text] = 8 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {5},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3823-9},
Abstract = {Searches for pair-produced scalar leptoquarks are performed
using 20 fb[Formula: see text] of proton-proton collision
data provided by the LHC and recorded by the ATLAS detector
at [Formula: see text] TeV. Events with two electrons
(muons) and two or more jets in the final state are used to
search for first (second)-generation leptoquarks. The
results from two previously published ATLAS analyses are
interpreted in terms of third-generation leptoquarks
decaying to [Formula: see text] and [Formula: see text]
final states. No statistically significant excess above the
Standard Model expectation is observed in any channel and
scalar leptoquarks are excluded at 95 % CL with masses up
to [Formula: see text] 1050 GeV for first-generation
leptoquarks, [Formula: see text] 1000 GeV for
second-generation leptoquarks, [Formula: see text] 625 GeV
for third-generation leptoquarks in the [Formula: see
text] channel, and 200 [Formula: see text] 640 GeV in
the [Formula: see text] channel.},
Doi = {10.1140/epjc/s10052-015-3823-9},
Key = {fds321205}
}
@article{fds221268,
Author = {CDF collaboration},
Title = {Searches for the Higgs boson decaying to
W+W−→ℓ+νℓ−ν¯ with the CDF II
detector},
Journal = {Phys.Rev.D88 (2013) 052012},
Year = {2013},
Month = {May},
Abstract = {http://prd.aps.org/abstract/PRD/v88/i5/e052012},
Key = {fds221268}
}
@article{fds308314,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bertoli, G and Bhatti, A and Bland, KR and Blumenfeld,
B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci, MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina,
K},
Title = {Searches for the Higgs boson decaying to W+W
-→ℓ+νℓ-ν̄ with the
CDF II detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.88.052012},
Abstract = {We present a search for a standard model Higgs boson
decaying to two W bosons that decay to leptons using the
full data set collected with the CDF II detector in
√s=1.96 TeV pp̄ collisions at the Fermilab Tevatron,
corresponding to an integrated luminosity of 9.7 fb-1. We
obtain no evidence for production of a standard model Higgs
boson with mass between 110 and 200 GeV/c2, and place upper
limits on the production cross section within this range. We
exclude standard model Higgs boson production at the 95%
confidence level in the mass range between 149 and 172
GeV/c2, while expecting to exclude, in the absence of
signal, the range between 155 and 175 GeV/c2. We also
interpret the search in terms of standard model Higgs boson
production in the presence of a fourth generation of
fermions and within the context of a fermiophobic Higgs
boson model. For the specific case of a standard-model-like
Higgs boson in the presence of fourth-generation fermions,
we exclude at the 95% confidence level Higgs boson
production in the mass range between 124 and 200 GeV/c2,
while expecting to exclude, in the absence of signal, the
range between 124 and 221 GeV/c2. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.052012},
Key = {fds308314}
}
@article{fds308558,
Author = {Aaltonen, T and others},
Title = {Searching the inclusive ℓγE̸T+b-quark signature for
radiative top quark decay and non-standard-model
processes},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {1},
Pages = {011102},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.011102},
Abstract = {We compare the inclusive production of events containing a
lepton (ℓ), a photon (γ), significant transverse momentum
imbalance (E̸T), and a jet identified as containing a
b-quark, to SM predictions. The search uses data produced in
proton-antiproton collisions at sqrt[s]=1.96 TeV
corresponding to 1.9 fb-1 of integrated luminosity
taken with the CDF detector. We find 28 ℓγbE̸T events
versus an expectation of 31.0-3.5+4.1 events. If we further
require events to contain at least three jets and large
total transverse energy, the largest SM source is radiative
top-quark pair production, tt̅ +γ. In the data we observe
16 tt̅ γ candidate events versus an expectation from SM
sources of 11.2-2.1+2.3. Assuming the difference between the
observed number and the predicted non-top-quark total of
6.8-2.0+2.2 is due to SM top-quark production, we estimate
the tt̅ γ cross section to be 0.15 ±
0.08 pb.},
Doi = {10.1103/PhysRevD.80.011102},
Key = {fds308558}
}
@article{fds308743,
Author = {Akimoto, T and Aoki, M and Hara, K and Kim, S and Nakamura, Y and Yoshitama, H and Azzi, P and Bacchetta, N and Bisello, D and Busetto, G and Manea, C and Pantano, D and Wang, Z and Behari, S and Maksimovic, P and Nord, B and Pursley, J and Schuyler, B and Benjamin, D and Cabrera, S and Kruse, M and Bolla, G and Bortoletto, D and Canepa, A and Fernandez, JP and Novak, J and Booth, P and Cooke, P and Burghard, A and Gorelov, I and Hoeferkamp, M and Naoumov, D and Seidel, S and Watje, P and Cardoso, G and Derylo, G and Fang, I and Flaugher, B and Hoff, J and Hrycyk, M and Lukens,
P and Merkel, P and Moccia, S and Nelson, T and Orlov, Y and Pavlicek, V and Shenai, A and Wester, W and Yarema, R and Yun, JC and Zimmerman, T and Chertok, M and Holbrook, B and Lander, R and Landry, T and Pellett, D and Soha, A and Yao, W and Ciobanu, CI and Hsiung, TH and Junk, T and Feng, EJ and Freeman, J and Galtieri, L and Garcia-Sciveres, M and Haber, C and Krieger, B and Lujan, PJ and Mandelli, E and von der Lippe, H and Walder, JP and Weber, M and Zetti, F and Zimmermann, S and Galyardt, J and Giurgiu, G and Hale, D and Hill, C and Incandela, J and Kyre, S and Stuart,
D and Harr, R and Hong, SC and Jeon, EJ and Joo, KK and Kong, DJ and Lee, J and Min, SN and Yang, YC and Kahkola, H and Karjalainen, S and Tavi, M and Kobayashi, K and Nakano, I and Tanaka, R and Lauhakangas, R and Orava,
R and Osterberg, K and Riipinen, P},
Title = {Sensors for the CDF Run2b silicon detector},
Journal = {IEEE Transactions on Nuclear Science},
Volume = {51},
Number = {4 I},
Pages = {1546-1554},
Publisher = {Institute of Electrical and Electronics Engineers
(IEEE)},
Year = {2004},
Month = {August},
url = {http://dx.doi.org/10.1109/TNS.2004.832586},
Abstract = {We describe the characteristics of silicon microstrip
sensors fabricated by Hamamatsu Photonics for the CDF Run 2b
silicon detector. A total of 953 sensors, including 117
prototype sensors, have been produced and tested. Five
sensors were irradiated with neutrons up to 1.4 × 1014
n/cm2 as a part of the sensor quality assurance program. The
electrical and mechanical characteristics are found to be
superior in all aspects and fulfill our specifications. We
comment on charge-up susceptibility of the sensors that
employ a (100) crystal structure.},
Doi = {10.1109/TNS.2004.832586},
Key = {fds308743}
}
@article{fds308319,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Signature-based search for delayed photons in exclusive
photon plus missing transverse energy events from pp̄
collisions with √s=1.96 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {3},
Pages = {031103},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.88.031103},
Abstract = {We present the first signature-based search for delayed
photons using an exclusive photon plus missing transverse
energy final state. Events are reconstructed in a data
sample from the CDF II detector corresponding to 6.3 fb-1 of
integrated luminosity from √s=1.96 TeV proton-antiproton
collisions. Candidate events are selected if they contain a
photon with an arrival time in the detector larger than
expected from a promptly produced photon. The mean number of
events from standard model sources predicted by the
data-driven background model based on the photon timing
distribution is 286±24. A total of 322 events are observed.
A p value of 12% is obtained, showing consistency of the
data with standard model predictions. © 2013 American
Physical Society.},
Doi = {10.1103/PhysRevD.88.031103},
Key = {fds308319}
}
@article{fds17503,
Author = {M.C. Kruse},
Title = {Silicon Detector Upgrades for the Tevatron Run
2},
Publisher = {Elsevier Science BV},
Year = {2002},
Month = {November},
url = {http://library.fnal.gov/archive/test-preprint/fermilab-conf-02-253-e.shtml},
Abstract = {http://library.fnal.gov/archive/test-preprint/fermilab-conf-02-253-e.shtml},
Key = {fds17503}
}
@article{fds308755,
Author = {Kruse, MC},
Title = {Silicon detector upgrades for the Tevatron Run
2},
Journal = {Nuclear Physics B - Proceedings Supplements},
Volume = {117},
Number = {SUPPL. 1},
Pages = {885-887},
Publisher = {Elsevier BV},
Year = {2003},
Month = {January},
url = {http://dx.doi.org/10.1016/S0920-5632(03)90698-0},
Abstract = {The current silicon devices being used by the DØ and CDF
collaborations for the Tevatron Run 2a, which is expected to
end in 2005 after accumulating about 2 fb-1 of data, will
need to be replaced due to radiation damage for the
following data collection period designated as Run 2b. We
will discuss these silicon replacement plans, the more
uniform design of the detectors between DØ and CDF, and the
current status of their fabrication.},
Doi = {10.1016/S0920-5632(03)90698-0},
Key = {fds308755}
}
@article{fds321264,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Simultaneous measurements of the tt¯, W+W-, and Z/γ∗
→ττ production cross-sections in pp collisions at √s
=7 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.91.052005},
Abstract = {Simultaneous measurements of the tt¯, W+W-, and
Z/γ∗→ττ production cross-sections using an integrated
luminosity of 4.6 fb-1 of pp collisions at √s=7 TeV
collected by the ATLAS detector at the LHC are presented.
Events are selected with two high transverse momentum
leptons consisting of an oppositely charged electron and
muon pair. The three processes are separated using the
distributions of the missing transverse momentum of events
with zero and greater than zero jet multiplicities.
Measurements of the fiducial cross-section are presented
along with results that quantify for the first time the
underlying correlations in the predicted and measured
cross-sections due to proton parton distribution functions.
These results indicate that the correlated
next-to-leading-order predictions for tt¯ and
Z/γ∗→ττ underestimate the data, while those at
next-to-next-to-leading-order generally describe the data
well. The full cross-sections are measured to be
σ(tt¯)=181.2±2.8-9.5+9.7±3.3±3.3 pb,
σ(W+W-)=53.3±2.7-8.0+7.3±1.0±0.5 pb, and
σ(Z/γ∗→ττ)=1174±24-87+72±21±9 pb, where the cited
uncertainties are due to statistics, systematic effects,
luminosity and the LHC beam energy measurement,
respectively. The W+W- measurement includes the small
contribution from Higgs boson decays, H→W+W-.},
Doi = {10.1103/PhysRevD.91.052005},
Key = {fds321264}
}
@article{fds308764,
Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Amaral, P and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and de
Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl,
A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett,
K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan,
AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung,
JY and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly,
A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R and Dagenhart, D},
Title = {Soft and hard interactions in [Formula Presented] collisions
at [Formula Presented] and 630 GeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {65},
Number = {7},
Pages = {12},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.65.072005},
Abstract = {We present a study of (Formula presented) collisions at
(Formula presented) and 630 GeV collected using a minimum
bias trigger by the CDF experiment in which the data set is
divided into two classes corresponding to “soft” and
“hard” interactions. For each subsample, the analysis
includes measurements of the multiplicity, transverse
momentum (Formula presented) spectrum, and the average
(Formula presented) and event-by-event (Formula presented)
dispersion as a function of multiplicity. A comparison of
results shows distinct differences in the behavior of the
two samples as a function of the center of mass (c.m.)
energy. We find evidence that the properties of the soft
sample are invariant as a function of c.m. energy. © 2002
The American Physical Society.},
Doi = {10.1103/PhysRevD.65.072005},
Key = {fds308764}
}
@article{fds376901,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye,
T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja,
S and Ai, X and Aielli, G and Aikot, A and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Cardoso, MA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler,
A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo,
MA and Bella, LA},
Title = {Software Performance of the ATLAS Track Reconstruction for
LHC Run 3},
Journal = {Computing and Software for Big Science},
Volume = {8},
Number = {1},
Year = {2024},
Month = {December},
url = {http://dx.doi.org/10.1007/s41781-023-00111-y},
Abstract = {Charged particle reconstruction in the presence of many
simultaneous proton–proton (pp) collisions in the LHC is a
challenging task for the ATLAS experiment’s reconstruction
software due to the combinatorial complexity. This paper
describes the major changes made to adapt the software to
reconstruct high-activity collisions with an average of 50
or more simultaneous pp interactions per bunch crossing
(pile-up) promptly using the available computing resources.
The performance of the key components of the track
reconstruction chain and its dependence on pile-up are
evaluated, and the improvement achieved compared to the
previous software version is quantified. For events with an
average of 60pp collisions per bunch crossing, the updated
track reconstruction is twice as fast as the previous
version, without significant reduction in reconstruction
efficiency and while reducing the rate of combinatorial fake
tracks by more than a factor two.},
Doi = {10.1007/s41781-023-00111-y},
Key = {fds376901}
}
@booklet{Baxter90,
Author = {Baxter, AM and Byrne, AP and Dracoulis, GD and Bark, RA and Riess, F and Stuchbery, AE and Kruse, MC and Poletti, AR},
Title = {Spectroscopy of high-spin states of po-206},
Journal = {Nuclear Physics A},
Volume = {515},
Number = {3},
Pages = {493-524},
Year = {1990},
Month = {September},
url = {http://dx.doi.org/10.1016/0375-9474(90)90595-D},
Abstract = {The yrast and near-yrast energy levels of 206Po have been
investigated to over 9 MeV excitation and up to spins of 24.
The measurements consisted of γγ-coincidence data,
internal-conversion-electron spectra, time spectra of
γ-rays relative to a pulsed beam, excitation functions and
γ-ray angular distributions. Two new isomers, with
lifetimes in the 1 ns range, were found. The observed level
structure is compared with the predictions of empirical
shell-model calculations in which 206Po is regarded as a
208Pb core with two valence protons and four valence neutron
holes. The agreement is generally satisfactory for the
observed odd-parity levels and for even parity levels with J
> 12; those with J = 6-12 are better accounted for by weak
coupling of two valence protons to a 204Pb core in its 0+1
and 4+1 states. © 1990.},
Doi = {10.1016/0375-9474(90)90595-D},
Key = {Baxter90}
}
@article{fds316863,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Standalone vertex finding in the ATLAS muon
spectrometer},
Journal = {Journal of Instrumentation},
Volume = {9},
Number = {2},
Pages = {P02001-P02001},
Publisher = {IOP Publishing},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1088/1748-0221/9/02/P02001},
Abstract = {A dedicated reconstruction algorithm to find decay vertices
in the ATLAS muon spectrometer is presented. The algorithm
searches the region just upstream of or inside the muon
spectrometer volume for multi-particle vertices that
originate from the decay of particles with long decay paths.
The performance of the algorithm is evaluated using both a
sample of simulated Higgs boson events, in which the Higgs
boson decays to long-lived neutral particles that in turn
decay to bb final states, and pp collision data at √s = 7
TeV collected with the ATLAS detector at the LHC during
2011.},
Doi = {10.1088/1748-0221/9/02/P02001},
Key = {fds316863}
}
@article{fds375931,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira,
MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos,
P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat,
A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley,
JR and Batool, B and Battaglia, M and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer,
JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi,
G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya,
DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul,
A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird,
GA and Birman, M and Bisanz, T and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner,
L and Brenner, R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo
Garcia, L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi,
E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov,
MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A and Clark, PJ and Clavijo Columbie and JM and Clawson, SE and Clement, C},
Title = {Strong Constraints on Jet Quenching in Centrality-Dependent
p+Pb Collisions at 5.02 TeV from ATLAS.},
Journal = {Physical review letters},
Volume = {131},
Number = {7},
Pages = {072301},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.131.072301},
Abstract = {Jet quenching is the process of color-charged partons losing
energy via interactions with quark-gluon plasma droplets
created in heavy-ion collisions. The collective expansion of
such droplets is well described by viscous hydrodynamics.
Similar evidence of collectivity is consistently observed in
smaller collision systems, including pp and p+Pb collisions.
In contrast, while jet quenching is observed in Pb+Pb
collisions, no evidence has been found in these small
systems to date, raising fundamental questions about the
nature of the system created in these collisions. The ATLAS
experiment at the Large Hadron Collider has measured the
yield of charged hadrons correlated with reconstructed jets
in 0.36 nb^{-1} of p+Pb and 3.6 pb^{-1} of pp
collisions at 5.02 TeV. The yields of charged hadrons with
p_{T}^{ch}>0.5 GeV near and opposite in azimuth to jets
with p_{T}^{jet}>30 or 60 GeV, and the ratios of these
yields between p+Pb and pp collisions, I_{pPb}, are
reported. The collision centrality of p+Pb events is
categorized by the energy deposited by forward neutrons from
the struck nucleus. The I_{pPb} values are consistent with
unity within a few percent for hadrons with
p_{T}^{ch}>4 GeV at all centralities. These data
provide new, strong constraints that preclude almost any
parton energy loss in central p+Pb collisions.},
Doi = {10.1103/physrevlett.131.072301},
Key = {fds375931}
}
@article{fds321269,
Author = {Aaltonen, T and Alon, R and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Duchovni, E and Ebina, K and Edgar, R and Elagin,
A},
Title = {Studies of high-transverse momentum jet substructure and top
quarks produced in 1.96 TeV proton-antiproton
collisions},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {3},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.91.032006},
Abstract = {Results of a study of the substructure of the highest
transverse momentum (pT) jets observed by the CDF
Collaboration are presented. Events containing at least one
jet with pT>400GeV/c in a sample corresponding to an
integrated luminosity of 5.95fb-1, collected in 1.96 TeV
proton-antiproton collisions at the Fermilab Tevatron
collider, are selected. A study of the jet mass, angularity,
and planar-flow distributions is presented, and the
measurements are compared with predictions of perturbative
quantum chromodynamics. A search for boosted top-quark
production is also described, leading to a 95% confidence
level upper limit of 38 fb on the production cross section
of top quarks with pT>400GeV/c.},
Doi = {10.1103/PhysRevD.91.032006},
Key = {fds321269}
}
@article{fds375928,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH},
Title = {Studies of the muon momentum calibration and performance of
the ATLAS detector with pp collisions at √s=13
TeV},
Journal = {European Physical Journal C},
Volume = {83},
Number = {8},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11584-x},
Abstract = {This paper presents the muon momentum calibration and
performance studies for the ATLAS detector based on the pp
collisions data sample produced at s = 13 TeV at the LHC
during Run 2 and corresponding to an integrated luminosity
of 139 fb - 1 . An innovative approach is used to correct
for potential charge-dependent momentum biases related to
the knowledge of the detector geometry, using the Z→
μ+μ- resonance. The muon momentum scale and resolution are
measured using samples of J/ ψ→ μ+μ- and Z→ μ+μ-
events. A calibration procedure is defined and applied to
simulated data to match the performance measured in real
data. The calibration is validated using an independent
sample of Υ → μ+μ- events. At the Z (J/ ψ) peak, the
momentum scale is measured with an uncertainty at the 0.05%
(0.1%) level, and the resolution is measured with an
uncertainty at the 1.5% (2%) level. The charge-dependent
bias is removed with a dedicated in situ correction for
momenta up to 450 GeV with a precision better than 0.03 TeV
- 1 .},
Doi = {10.1140/epjc/s10052-023-11584-x},
Key = {fds375928}
}
@article{fds321237,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Study of (W/Z)H production and Higgs boson couplings using
H→ W W∗ decays with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {8},
Publisher = {Springer Nature},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2015)137},
Abstract = {Abstract: A search for Higgs boson production in association
with a W or Z boson, in the H→ W W∗ decay channel, is
performed with a data sample collected with the ATLAS
detector at the LHC in proton-proton collisions at
centre-of-mass energies √s=7$$ \sqrt{s}=7 $$ TeV and 8
TeV, corresponding to integrated luminosities of 4.5 fb−1
and 20.3 fb−1, respectively. The WH production mode is
studied in two-lepton and three-lepton final states, while
two- lepton and four-lepton final states are used to search
for the ZH production mode. The observed significance, for
the combined W H and ZH production, is 2.5 standard
deviations while a significance of 0.9 standard deviations
is expected in the Standard Model Higgs boson hypothesis.
The ratio of the combined W H and ZH signal yield to the
Standard Model expectation, μV H , is found to be μV H =
3.0− 1.1+ 1.3(stat.)− 0.7+ 1.0(sys.) for the Higgs boson
mass of 125.36 GeV. The W H and ZH production modes are also
combined with the gluon fusion and vector boson fusion
production modes studied in the H → W W∗ → ℓνℓν
decay channel, resulting in an overall observed significance
of 6.5 standard deviations and μggF + VBF + VH = 1. 16−
0.15+ 0.16(stat.)− 0.15+ 0.18(sys.). The results are
interpreted in terms of scaling factors of the Higgs boson
couplings to vector bosons (κV ) and fermions (κF ); the
combined results are: |κV| = 1.06− 0.10+ 0.10, |κF| = 0.
85− 0.20+ 0.26.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP08(2015)137},
Key = {fds321237}
}
@article{fds308769,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Dominguez, A and Donati,
S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erbacher, R and Errede, D and Errede, S and Fan,
Q and Fang, HC and Feild, RG and Fernandez, JP and Ferretti, C and Field,
RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman,
J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov,
I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian,
G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa,
T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huffman, BT and Hughes, R and Huston,
J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon,
T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim,
MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis,
JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima,
K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto,
WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt,
M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel,
S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding,
J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda,
H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
F and Vaiciulis, T and Valls, J and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters,
D and Watts, T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Study of B0 → J/ψK(*)0π+π-
decays with the collider detector at Fermilab},
Journal = {Physical Review Letters},
Volume = {88},
Number = {7},
Pages = {718011-718016},
Year = {2002},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.88.071801},
Abstract = {The study of the decays B0 → J/ψK(*)0 π+π-, was
reported. The study involved the creation of a uū or dd̄
quark pair in addition to a b̄ → c̄(cs̄) decay.
Three-level dimuon trigger was used in the analysis. Events
with two separate sets of atleast three linked hits in the
muon chambers. The second level required drift chamber
tracks with pT > 2.0 GeV/c. J/ψ → μ+μ- candidates,
were accepted in the third level, with a reconstructed
invariant mass between 2.8 and 3.8 GeV/c2.},
Doi = {10.1103/physrevlett.88.071801},
Key = {fds308769}
}
@article{fds321151,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Study of hard double-parton scattering in four-jet events in
pp collisions at √s=7 TeV with the ATLAS
experiment},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {11},
Publisher = {Springer Nature},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2016)110},
Abstract = {Inclusive four-jet events produced in proton-proton
collisions at a centre-of-mass energy of s=7 TeV are
analysed for the presence of hard double-parton scattering
using data corresponding to an integrated luminosity of 37.3
pb−1, collected with the ATLAS detector at the LHC. The
contribution of hard double-parton scattering to the
production of four-jet events is extracted using an
artificial neural network, assuming that hard double-parton
scattering can be approximated by an uncorrelated overlaying
of dijet events. For events containing at least four jets
with transverse momentum pT ≥ 20 GeV and pseudorapidity
|η| ≤ 4.4, and at least one having pT ≥ 42.5 GeV, the
contribution of hard double-parton scattering is estimated
to be fDPS = 0.092− 0.011+ 0.005(stat.)− 0.037+
0.033(syst.). After combining this measurement with those of
the inclusive dijet and four-jet cross-sections in the
appropriate phase space regions, the effective
cross-section, σeff , was determined to be σeff = 14. 9−
1.0+ 1.2(stat.)− 3.8+ 5.1(syst.) mb. This result is
consistent within the quoted uncertainties with previous
measurements of σeff , performed at centre-of-mass energies
between 63 GeV and 8 TeV using various final states, and it
corresponds to 21− 6+ 7 % of the total inelastic
cross-section measured at s=7 TeV. The distributions of the
observables sensitive to the contribution of hard
double-parton scattering, corrected for detector effects,
are also provided.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP11(2016)110},
Key = {fds321151}
}
@article{fds308278,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E and Arik, M and Armbruster, AJ},
Title = {Study of heavy-flavor quarks produced in association with
top-quark pairs at s =7TeV using the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.89.072012},
Abstract = {Using a sample of dilepton top-quark pair (tt̄) candidate
events, a study is performed of the production of top-quark
pairs together with heavy-flavor (HF) quarks, the sum of
tt̄+b+X and tt̄+c+X, collectively referred to as tt̄+HF.
The data set used corresponds to an integrated luminosity of
4.7fb-1 of proton-proton collisions at a center-of-mass
energy of 7 TeV recorded by the ATLAS detector at the CERN
Large Hadron Collider. The presence of additional HF (b or
c) quarks in the tt̄ sample is inferred by looking for
events with at least three b-tagged jets, where two are
attributed to the b quarks from the tt̄ decays and the
third to additional HF production. The dominant background
to tt̄+HF in this sample is tt̄+jet events in which a
light-flavor jet is misidentified as a heavy-flavor jet. To
determine the heavy- and light-flavor content of the
additional b-tagged jets, a fit to the vertex mass
distribution of b-tagged jets in the sample is performed.
The result of the fit shows that 79±14(stat)±22(syst) of
the 105 selected extra b-tagged jets originate from HF
quarks, 3 standard deviations away from the hypothesis of
zero tt̄+HF production. The result for extra HF production
is quoted as a ratio (RHF) of the cross section for tt̄+HF
production to the cross section for tt̄ production with at
least one additional jet. Both cross sections are measured
in a fiducial kinematic region within the ATLAS acceptance.
RHF is measured to be [6.2±1.1(stat)±1.8(syst)]% for jets
with pT>25GeV and |η|<2.5, in agreement with the
expectations from Monte Carlo generators. © 2014 CERN, for
the ATLAS Collaboration.},
Doi = {10.1103/PhysRevD.89.072012},
Key = {fds308278}
}
@article{fds376902,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V},
Title = {Study of High-Transverse-Momentum Higgs Boson Production in
Association with a Vector Boson in the qqbb Final State with
the ATLAS Detector},
Journal = {Physical Review Letters},
Volume = {132},
Number = {13},
Year = {2024},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevLett.132.131802},
Abstract = {This Letter presents the first study of Higgs boson
production in association with a vector boson (V ¼ W or Z)
in the fully hadronic qqbb final state using data recorded
by the ATLAS detector at the LHC in proton-proton collisions
at √s = 13 TeV and corresponding to an integrated
luminosity of 137 fb−1. The vector bosons and Higgs bosons
are each reconstructed as large-radius jets and tagged using
jet substructure techniques. Dedicated tagging algorithms
exploiting b-tagging properties are used to identify jets
consistent with Higgs bosons decaying into bb̄. Dominant
backgrounds from multijet production are determined directly
from the data, and a likelihood fit to the jet mass
distribution of Higgs boson candidates is used to extract
the number of signal events. The VH production cross section
is measured inclusively and differentially in several ranges
of Higgs boson transverse momentum: 250–450, 450–650,
and greater than 650 GeV. The inclusive signal yield
relative to the standard model expectation is observed to be
μ = 1.4+1.0−0.9 and the corresponding cross section is
3.1 ± 1.3(stat)+1.8−1.4(syst) pb.},
Doi = {10.1103/PhysRevLett.132.131802},
Key = {fds376902}
}
@article{fds308718,
Author = {Acosta, and D, and others},
Title = {Study of jet shapes in inclusive jet production in p anti-p
collisions at s**(1/2) = 1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D71},
Number = {11},
Pages = {112002},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.112002},
Abstract = {http://arxiv.org/abs/hep-ex/0505013},
Doi = {10.1103/PhysRevD.71.112002},
Key = {fds308718}
}
@article{fds308504,
Author = {Aaltonen, and T, and others},
Title = {Study of multi-muon events produced in $p \bar{p}$
interactions at $\sqrt{s} = 1.96$-TeV},
Journal = {Eur. Phys. J.},
Volume = {C68},
Number = {1},
Pages = {109-118},
Publisher = {Springer Nature},
Year = {2010},
url = {http://dx.doi.org/10.1140/epjc/s10052-010-1336-0},
Abstract = {We report the results of a study of multi-muon events
produced at the Fermilab Tevatron collider and acquired with
the CDF II detector using a dedicated dimuon trigger. The
production cross section and kinematics of events in which
both muon candidates are produced inside the beam pipe of
radius 1.5 cm are successfully modeled by known processes
which include heavy flavor production. In contrast, we are
presently unable to fully account for the number and
properties of the remaining events, in which at least one
muon candidate is produced outside of the beam pipe, in
terms of the same understanding of the CDF II detector,
trigger, and event reconstruction. © 2010 The
Author(s).},
Doi = {10.1140/epjc/s10052-010-1336-0},
Key = {fds308504}
}
@article{fds321612,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Study of orbitally excited B mesons and evidence for a new
Bπ resonance},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {1},
Pages = {012013},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.90.012013},
Abstract = {Using the full CDF Run II data sample, we report evidence
for a new resonance, which we refer to as B(5970), found
simultaneously in the B0π+ and B+π- mass distributions
with a significance of 4.4 standard deviations. We further
report the first study of resonances consistent with
orbitally excited B+ mesons and an updated measurement of
the properties of orbitally excited B0 and Bs0 mesons. We
measure the masses and widths of all states, as well as the
relative production rates of the B1, B2*, and B(5970) states
and the branching fraction of the Bs2*0 state to either
B*+K- and B+K-. Furthermore, we measure the production rates
of the orbitally excited B0,+ states relative to the B0,+
ground state. The masses of the new B(5970) resonances are
5978±5(stat)±12(syst)MeV/c2 for the neutral state and
5961±5(stat)±12(syst)MeV/c2 for the charged state,
assuming that the resonance decays into Bπ final states.
The properties of the orbitally excited and the new
B(5970)0,+ states are compatible with isospin symmetry. ©
2014 American Physical Society.},
Doi = {10.1103/PhysRevD.90.012013},
Key = {fds321612}
}
@article{fds308398,
Author = {Aaltonen, T and Alon, R and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi,
J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli,
M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar,
C and Cuevas, J and Culbertson, R},
Title = {Study of substructure of high transverse momentum jets
produced in proton-antiproton collisions at
√s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.85.091101},
Abstract = {A study of the substructure of jets with transverse momentum
greater than 400GeV/c produced in proton-antiproton
collisions at a center-of-mass energy of 1.96 TeV at the
Fermilab Tevatron Collider and recorded by the CDF II
detector is presented. The distributions of the jet mass,
angularity, and planar flow are measured for the first time
in a sample with an integrated luminosity of 5.95fb -1. The
observed substructure for high mass jets is consistent with
predictions from perturbative quantum chromodynamics. ©
2012 American Physical Society.},
Doi = {10.1103/PhysRevD.85.091101},
Key = {fds308398}
}
@article{fds308890,
Author = {al, FAE},
Title = {Study of t(t)over-bar production in p(p)over-bar collisions
using total transverse energy},
Journal = {Phys. Rev. Lett.},
Volume = {75},
Number = {22},
Pages = {3997-4002},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.75.3997},
Abstract = {We analyze a sample of W+jet events collected with the
Collider Detector at Fermilab (CDF) in pp» collisions at
s=1.8 TeV to study tt» production. We employ a simple
kinematical variable H, defined as the scalar sum of the
transverse energies of the lepton, neutrino, and jets. For
events with a W boson and four or more jets, the shape of
the H distribution deviates by 3.8 standard deviations from
that expected from known backgrounds to tt» production.
However, this distribution agrees well with a linear
combination of background and tt» events, the agreement
being best for a top mass of 180 GeV/c2. © 1995 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.75.3997},
Key = {fds308890}
}
@article{fds30249,
Author = {CDF Collaboration},
Title = {Study of the Heavy Flavor Content of Jets Produced in
Association with W Bosons in P anti-P Collisions at s**(1/2)
= 1.8-TEV},
Journal = {Phys.Rev.D},
Volume = {65},
Number = {052007},
Year = {2002},
Key = {fds30249}
}
@article{fds308758,
Author = {al, DAE},
Title = {Study of the heavy flavor content of jets produced in
association with W bosons in pp collisions at $\sqrt{s} =
1.8 TeV},
Journal = {Physical Review},
Volume = {D65},
Number = {5},
Pages = {052006},
Publisher = {American Physical Society (APS)},
Year = {2002},
url = {http://dx.doi.org/10.1103/PhysRevD.65.052007},
Abstract = {We present a detailed examination of the heavy flavor
content of the W+jet data sample collected with the Collider
Detector at Fermilab during the 1992-1995 collider run at
the Fermilab Tevatron. Jets containing heavy flavor quarks
are selected via the identification of secondary vertices or
semileptonic decays of b and c quarks. There is generally
good agreement between the rates of secondary vertices and
soft leptons in the data and in the standard model
simulation including single and pair production of top
quarks. An exception is the number of events in which a
single jet has both a soft lepton and a secondary vertex
tag. In W+2,3 jet data, we find 13 such events where we
expected 4.4± 0.6 events. The kinematic properties of this
small sample of events are statistically difficult to
reconcile with the simulation of standard model
processes.},
Doi = {10.1103/PhysRevD.65.052007},
Key = {fds308758}
}
@article{fds321166,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán,
SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura,
P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A},
Title = {Study of the rare decays of [Formula: see text] and
[Formula: see text] into muon pairs from data collected
during the LHC Run 1 with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {9},
Pages = {513},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4338-8},
Abstract = {A study of the decays [Formula: see text] and [Formula: see
text] has been performed using data corresponding to an
integrated luminosity of 25 fb[Formula: see text] of 7 and
8 TeV proton-proton collisions collected with the ATLAS
detector during the LHC Run 1. For the [Formula: see text]
dimuon decay, an upper limit on the branching fraction is
set at [Formula: see text] at 95 % confidence level. For
[Formula: see text], the branching fraction [Formula: see
text] is measured. The results are consistent with the
Standard Model expectation with a <i>p</i> value of 4.8 %,
corresponding to 2.0 standard deviations.},
Doi = {10.1140/epjc/s10052-016-4338-8},
Key = {fds321166}
}
@article{fds308270,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Study of top quark production and decays involving a tau
lepton at CDF and limits on a charged Higgs boson
contribution},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.89.091101},
Abstract = {We present an analysis of top-antitop quark production and
decay into a tau lepton, tau neutrino, and bottom quark
using data from 9fb-1 of integrated luminosity at the
Collider Detector at Fermilab. Dilepton events, where one
lepton is an energetic electron or muon and the other a
hadronically decaying tau lepton, originating from
proton-antiproton collisions at s=1.96TeV, are used. A
top-antitop quark production cross section of 8.1±2.1pb is
measured, assuming standard-model top quark decays. By
separately identifying for the first time the single-tau and
the ditau components, we measure the branching fraction of
the top quark into the tau lepton, tau neutrino, and bottom
quark to be (9.6±2.8)%. The branching fraction of top quark
decays into a charged Higgs boson and a bottom quark, which
would imply violation of lepton universality, is limited to
be less than 5.9% at a 95% confidence level [for
B(H-→τν̄)=1]. © 2014 American Physical
Society.},
Doi = {10.1103/PhysRevD.89.091101},
Key = {fds308270}
}
@article{fds308498,
Author = {Aaltonen, and T, and others},
Title = {Studying the Underlying Event in Drell-Yan and High
Transverse Momentum Jet Production at the
Tevatron},
Journal = {Phys. Rev.},
Volume = {D82},
Number = {3},
Pages = {034001},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.82.034001},
Abstract = {http://arxiv.org/abs/1003.3146},
Doi = {10.1103/PhysRevD.82.034001},
Key = {fds308498}
}
@article{fds321221,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Summary of the ATLAS experiment’s sensitivity to
supersymmetry after LHC Run 1 — interpreted in the
phenomenological MSSM},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {10},
Publisher = {Springer Nature},
Year = {2015},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2015)134},
Abstract = {Abstract: A summary of the constraints from the ATLAS
experiment on R-parity-conserving supersymmetry is
presented. Results from 22 separate ATLAS searches are
considered, each based on analysis of up to 20.3 fb−1 of
proton-proton collision data at centre-of-mass energies of
s=7$$ \sqrt{s}=7 $$ and 8 TeV at the Large Hadron Collider.
The results are interpreted in the context of the
19-parameter phenomenological minimal supersymmetric
standard model, in which the lightest supersymmetric
particle is a neutralino, taking into account constraints
from previous precision electroweak and flavour measurements
as well as from dark matter related measurements. The
results are presented in terms of constraints on
supersymmetric particle masses and are compared to limits
from simplified models. The impact of ATLAS searches on
parameters such as the dark matter relic density, the
couplings of the observed Higgs boson, and the degree of
electroweak fine-tuning is also shown. Spectra for surviving
supersymmetry model points with low fine-tunings are
presented.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP10(2015)134},
Key = {fds321221}
}
@article{fds314187,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Summary of the searches for squarks and gluinos using √s =
8 TeV pp collisions with the ATLAS experiment at the
LHC},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {10},
Publisher = {Springer Nature},
Year = {2015},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2015)054},
Abstract = {Abstract: A summary is presented of ATLAS searches for
gluinos and first- and second-generation squarks in final
states containing jets and missing transverse momentum, with
or without leptons or b-jets, in the s=8$$ \sqrt{s}=8 $$ TeV
data set collected at the Large Hadron Collider in 2012.
This paper reports the results of new interpretations and
statistical combinations of previously published analyses,
as well as a new analysis. Since no significant excess of
events over the Standard Model expectation is observed, the
data are used to set limits in a variety of models. In all
the considered simplified models that assume R-parity
conservation, the limit on the gluino mass exceeds 1150 GeV
at 95% confidence level, for an LSP mass smaller than 100
GeV. Furthermore, exclusion limits are set for left-handed
squarks in a phenomenological MSSM model, a minimal
Supergravity/Constrained MSSM model, R-parity-violation
scenarios, a minimal gauge-mediated supersymmetry breaking
model, a natural gauge mediation model, a non-universal
Higgs mass model with gaugino mediation and a minimal model
of universal extra dimensions.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP10(2015)054},
Key = {fds314187}
}
@article{fds308911,
Author = {Azzi, P and Bacchetta, N and Barnett, BA and Bailey, M and Bedeschi, F and Bisello, D and Cammerata, JD and Carithers, WC and Chao, HY and Chiou,
CN and Cihangir, S and Ely, RP and Engels, E and Franceschi, A and Barbaro-Galtieri, A and Guerra, M and Garfinkel, AF and Gillespie, G and Glenzinski, D and Gonzalez, H and Gonzalez, S and Grimm, C and Haber, C and Hawke, T and Hrycyk, M and Incandela, J and Kajfasz, E and Klein, R and Kleinfelder, S and Kruse, M and Lundberg, B and Mando', F and Matthews,
J and Menzione, A and Nelson, C and Paccagnella, A and Paulini, M and Peters, MD and Praticelli, N and Raffaelli, F and Ratzmann, P and Schindler, A and Sciacca, FG and Scott, L and Shapiro, MD and Shaw, NM and Shaw, T and Shepard, P and Singh, P and Skarha, JE and Snider, FD and Song,
L and Spalding, J and Stuart, D and Tipton, P and Tkaczyk, S and Tollefson,
K and Tousignant, D and Turner, K and Wang, CH and Wang, MJ and Watts, G and Wenzel, H and Wu, SC and Yao, W and Yarema, R and Yun, JC and Zetti,
F},
Title = {SVX', the new CDF silicon vertex detector},
Journal = {Nuclear Inst. and Methods in Physics Research,
A},
Volume = {360},
Number = {1-2},
Pages = {137-140},
Publisher = {Elsevier BV},
Year = {1995},
Month = {June},
url = {http://dx.doi.org/10.1016/0168-9002(95)00087-9},
Abstract = {The Collider Detector at Fermilab (CDF) radiation hardened
silicon vertex detector (SVX') is described. The new
detector has several improvements over its predecessor such
as better signal to noise and higher efficiency. It is
expected to have a radiation tolerance in excess of 1 Mrad.
It has been taking data for several months and some
preliminary results are shown. © 1995.},
Doi = {10.1016/0168-9002(95)00087-9},
Key = {fds308911}
}
@article{fds375929,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari,
T and Barisits, M-S and Barklow, T and Barnett, RM and Baron, P and Baron
Moreno, DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Battulga, D and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram,
IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Bisceglie,
E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
JE and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock,
I and Brooijmans, G and Brooks, WK and Brost, E and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson,
BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter,
JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chiu, YH and Chizhov,
MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A and Clark, PJ and Clavijo Columbie,
JM},
Title = {Test of CP Invariance in Higgs Boson Vector-Boson-Fusion
Production Using the H→γγ Channel with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {6},
Pages = {061802},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.131.061802},
Abstract = {A test of CP invariance in Higgs boson production via
vector-boson fusion has been performed in the H→γγ
channel using 139 fb^{-1} of proton-proton collision
data at sqrt[s]=13 TeV collected by the ATLAS detector
at the LHC. The optimal observable method is used to probe
the CP structure of interactions between the Higgs boson and
electroweak gauge bosons, as described by an effective field
theory. No sign of CP violation is observed in the data.
Constraints are set on the parameters describing the
strength of the CP-odd component in the coupling between the
Higgs boson and the electroweak gauge bosons in two
effective field theory bases: d[over ˜] in the HISZ basis
and c_{HW[over ˜]} in the Warsaw basis. The results
presented are the most stringent constraints on CP violation
in the coupling between Higgs and weak bosons. The 95% C.L.
constraint on d[over ˜] is derived for the first time and
the 95% C.L. constraint on c_{HW[over ˜]} has been improved
by a factor of 5 compared to the previous
measurement.},
Doi = {10.1103/physrevlett.131.061802},
Key = {fds375929}
}
@article{fds322006,
Author = {Aad, G and Abbott, B and Abdinov, O and Abdallah, J and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund,
OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan,
AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel,
O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito,
L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas,
CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou,
Y},
Title = {Test of CP invariance in vector-boson fusion production of
the Higgs boson using the Optimal Observable method
in the ditau decay channel with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {12},
Pages = {658},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4499-5},
Abstract = {A test of CP invariance in Higgs boson production via
vector-boson fusion using the method of the <i>Optimal
Observable</i> is presented. The analysis exploits the decay
mode of the Higgs boson into a pair of [Formula: see text]
leptons and is based on 20.3 [Formula: see text] of
proton-proton collision data at [Formula: see text] =
8 [Formula: see text] collected by the ATLAS experiment at
the LHC. Contributions from CP-violating interactions
between the Higgs boson and electroweak gauge bosons are
described in an effective field theory framework, in which
the strength of CP violation is governed by a single
parameter [Formula: see text]. The mean values and
distributions of CP-odd observables agree with the
expectation in the Standard Model and show no sign of CP
violation. The CP-mixing parameter [Formula: see text] is
constrained to the interval [Formula: see text] at 68%
confidence level, consistent with the Standard Model
expectation of [Formula: see text].},
Doi = {10.1140/epjc/s10052-016-4499-5},
Key = {fds322006}
}
@article{fds365385,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Test of the universality of τ and μ lepton couplings in
W-boson decays with the ATLAS detector},
Journal = {Nature Physics},
Volume = {17},
Number = {7},
Pages = {813-818},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1038/s41567-021-01236-w},
Abstract = {The standard model of particle physics encapsulates our best
current understanding of physics at the smallest scales. A
fundamental axiom of this theory is the universality of the
couplings of the different generations of leptons to the
electroweak gauge bosons. The measurement of the ratio of
the decay rate of W bosons to τ leptons and muons,
R(τ/μ), constitutes an important test of this axiom. Using
139 fb−1 of proton–proton collisions recorded with the
ATLAS detector at a centre-of-mass energy of 13 TeV, we
report a measurement of this quantity from di-leptonic tt¯
events where the top quarks decay into a W boson and a
bottom quark. We can distinguish muons originating from W
bosons and those originating from an intermediate τ lepton
through the muon transverse impact parameter and differences
in the muon transverse momentum spectra. The measured value
of R(τ/μ) is 0.992 ± 0.013 [± 0.007(stat) ±
0.011(syst)] and is in agreement with the hypothesis of
universal lepton couplings as postulated in the standard
model. This is the only such measurement from the Large
Hadron Collider, so far, and obtains twice the precision of
previous measurements.},
Doi = {10.1038/s41567-021-01236-w},
Key = {fds365385}
}
@article{fds308782,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Bruner,
N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang,
PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin,
T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Errede, D and Errede, S and Fan, Q and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Gorelov, I and Giromini, P and Glagolev,
V and Gold, M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Gris, P and Groer, L and Grosso-Pilcher,
C and Guenther, M and Guillian, G and Costa, JGD and Guo, RS and Haas, RM and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss,
A and Herndon, M and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn,
P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korn,
A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte,
T and Lee, AM and Lee, K and Leone, S and Lewis, JD and Lindgren, M and Liss,
TM and Liu, JB and Liu, YC and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak,
R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer,
J and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nahn, S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Nelson, T and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari,
F and Paoletti, R and Papadimitriou, V and Pappas, SP and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos, A and Pondrom,
L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos,
F and Pukhov, O and Punzi, G and Ragan, K and Rakitine, A and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Rossin, R and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt,
M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel,
S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
M and Spiegel, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda,
H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
F and Vaiciulis, T and Valls, J and Vejcik, S and Velev, G and Vidal, R and Vilar, R and Volobouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang,
MJ and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Williams, HH and Wilson,
P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh,
GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu,
Z and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Tests of enhanced leading order QCD in W boson plus jets
events from 1.8 TeV p̄p collisions},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {63},
Number = {7},
Pages = {720031-7200329},
Year = {2001},
ISSN = {0556-2821},
Abstract = {We present a study of events with W bosons and hadronic jets
produced in p̄p collisions at a center of mass energy of
1.8 TeV. The data consist of 51400 W → e ν decay
candidates from 108 pb-1 of integrated luminosity collected
using the CDF detector at the Fermilab Tevatron collider.
Cross sections and jet production properties have been
measured for W + ≥ 1 to ≥ 4 jet events. The data compare
well to predictions of leading-order QCD matrix element
calculations with added gluon radiation and simulated parton
fragmentation.},
Key = {fds308782}
}
@article{fds314170,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox,
CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson,
R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de
Barbaro, P and de Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto,
F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, A and Evdokimov, VN and Farrington,
S and Fauré, A and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov, V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gogota, O and Gold, M and Goldin, D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López,
O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da
Costa, J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Hedin,
D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere, A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun,
SY and Jung, AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kaur, M and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich, I and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster, M and Lannon, K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li, H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour, J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega, J and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta, A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett, J and Neu, C and Neustroev, P},
Title = {Tevatron Combination of Single-Top-Quark Cross Sections and
Determination of the Magnitude of the Cabibbo-Kobayashi-Maskawa
Matrix Element V_{tb}.},
Journal = {Physical review letters},
Volume = {115},
Number = {15},
Pages = {152003},
Year = {2015},
Month = {October},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.115.152003},
Abstract = {We present the final combination of CDF and D0 measurements
of cross sections for single-top-quark production in
proton-antiproton collisions at a center-of-mass energy of
1.96 TeV. The data correspond to total integrated
luminosities of up to 9.7 fb^{-1} per experiment. The
t-channel cross section is measured to be
σ_{t}=2.25_{-0.31}^{+0.29} pb. We also present the
combinations of the two-dimensional measurements of the s-
vs t-channel cross section. In addition, we give the
combination of the s+t channel cross section measurement
resulting in σ_{s+t}=3.30_{-0.40}^{+0.52} pb, without
assuming the standard model value for the ratio
σ_{s}/σ_{t}. The resulting value of the magnitude of the
top-to-bottom quark coupling is |V_{tb}|=1.02_{-0.05}^{+0.06},
corresponding to |V_{tb}|>0.92 at the 95%
C.L.},
Doi = {10.1103/physrevlett.115.152003},
Key = {fds314170}
}
@article{fds321256,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox,
CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson,
R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de
Barbaro, P and de Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto,
F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, VN and Farrington, S and Fauré, A and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field,
R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest,
R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov, V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini,
P and Glagolev, V and Glenzinski, D and Gogota, O and Gold, M and Goldin,
D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald,
MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr,
RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays,
C and Hays, J and Head, T and Hebbeker, T and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De
La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere,
A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung,
AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kaur, M and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich,
I and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg,
J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster,
M and Lannon, K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee,
SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis,
JD and Li, D and Li, H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour, J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega, J and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta, A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett, J and Neu, C and Neustroev, P and Nguyen, HT},
Title = {Tevatron constraints on models of the Higgs boson with
exotic spin and parity using decays to bottom-antibottom
quark pairs.},
Journal = {Physical review letters},
Volume = {114},
Number = {15},
Pages = {151802},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.114.151802},
Abstract = {Combined constraints from the CDF and D0 Collaborations on
models of the Higgs boson with exotic spin J and parity P
are presented and compared with results obtained assuming
the standard model value JP=0+. Both collaborations analyzed
approximately 10 fb(-) of proton-antiproton collisions
with a center-of-mass energy of 1.96 TeV collected at the
Fermilab Tevatron. Two models predicting exotic Higgs bosons
with JP=0- and JP=2+ are tested. The kinematic properties of
exotic Higgs boson production in association with a vector
boson differ from those predicted for the standard model
Higgs boson. Upper limits at the 95% credibility level on
the production rates of the exotic Higgs bosons, expressed
as fractions of the standard model Higgs boson production
rate, are set at 0.36 for both the JP=0- hypothesis and the
JP=2+ hypothesis. If the production rate times the branching
ratio to a bottom-antibottom pair is the same as that
predicted for the standard model Higgs boson, then the
exotic bosons are excluded with significances of 5.0
standard deviations and 4.9 standard deviations for the
JP=0- and JP=2+ hypotheses, respectively.},
Doi = {10.1103/physrevlett.114.151802},
Key = {fds321256}
}
@article{fds365392,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Alison, J and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Anderson, JT and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira,
RA},
Title = {The ATLAS fast TracKer system},
Journal = {Journal of Instrumentation},
Volume = {16},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1088/1748-0221/16/07/P07006},
Abstract = {The ATLAS Fast TracKer (FTK) was designed to provide full
tracking for the ATLAS high-level trigger by using pattern
recognition based on Associative Memory (AM) chips and
fitting in high-speed field programmable gate arrays. The
tracks found by the FTK are based on inputs from all modules
of the pixel and silicon microstrip trackers. The as-built
FTK system and components are described, as is the online
software used to control them while running in the ATLAS
data acquisition system. Also described is the simulation of
the FTK hardware and the optimization of the AM pattern
banks. An optimization for long-lived particles with large
impact parameter values is included. A test of the FTK
system with the data playback facility that allowed the FTK
to be commissioned during the shutdown between Run 2 and Run
3 of the LHC is reported. The resulting tracks from part of
the FTK system covering a limited η-ϕ region of the
detector are compared with the output from the FTK
simulation. It is shown that FTK performance is in good
agreement with the simulation.},
Doi = {10.1088/1748-0221/16/07/P07006},
Key = {fds365392}
}
@article{fds365360,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C and Arce, ATH and Arguin, JF},
Title = {The ATLAS inner detector trigger performance in pp
collisions at 13 TeV during LHC Run 2},
Journal = {European Physical Journal C},
Volume = {82},
Number = {3},
Year = {2022},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09920-0},
Abstract = {The design and performance of the inner detector trigger for
the high level trigger of the ATLAS experiment at the Large
Hadron Collider during the 2016–2018 data taking period is
discussed. In 2016, 2017, and 2018 the ATLAS detector
recorded 35.6fb-1, 46.9fb-1, and 60.6fb-1 respectively of
proton–proton collision data at a centre-of-mass energy of
13 TeV. In order to deal with the very high interaction
multiplicities per bunch crossing expected with the 13 TeV
collisions the inner detector trigger was redesigned during
the long shutdown of the Large Hadron Collider from 2013
until 2015. An overview of these developments is provided
and the performance of the tracking in the trigger for the
muon, electron, tau and b-jet signatures is discussed. The
high performance of the inner detector trigger with these
extreme interaction multiplicities demonstrates how the
inner detector tracking continues to lie at the heart of the
trigger performance and is essential in enabling the ATLAS
physics programme.},
Doi = {10.1140/epjc/s10052-021-09920-0},
Key = {fds365360}
}
@article{fds308821,
Author = {Azzi-Bacchetta, P and Bacchetta, N and Basti, A and Bedeschi, F and Bisello, D and Blusk, S and Chertok, M and Chiarelli, G and Demina, R and Donati, S and Field, R and Galtieri, L and Goldstein, J and Grim, G and Guerzoni, M and Haber, C and Hara, K and Hartmann, F and Heiss, A and Hill,
C and Hrycyk, M and Incandela, J and Kato, Y and Kim, BJ and Knoblauch, D and Kruse, M and Lei, CM and Leone, S and Martignon, G and Mcyntire, P and Miyazaky, Y and Moggi, A and Muller, T and Munar-Ara, A and Okusawa, T and Palmonari, F and Pellett, D and Piacentino, G and Raffaelli, F and Saltzberg, D and Sanders, E and Schilling, M and Shimojima, M and Stuart, D and Takano, T and Takikawa, K and Tipton, P and Turini, N and Wenzel, H and Zetti, F and Zucchelli, S},
Title = {The CDF Intermediate Silicon Layers detector},
Journal = {Nuclear Physics B - Proceedings Supplements},
Volume = {78},
Number = {1-3},
Pages = {307-310},
Publisher = {Elsevier BV},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1016/S0920-5632(99)00562-9},
Abstract = {The Intermediate Silicon Layers (ISL) detector is presently
being built as part of CDF upgrades. The ISL is a large
radius (28 cm) silicon tracker with a total active area of
about 3.5 m2. The challenge is to build a device which
provides precise 3D points introducing a minimal amount of
material for the supporting structure. The design and the
status of the project are described.},
Doi = {10.1016/S0920-5632(99)00562-9},
Key = {fds308821}
}
@article{fds308818,
Author = {Affolder, A and Azzi-Bacchetta, P and Bacchetta, N and Barbaro-Galtieri, A and Barker, G and Basti, A and Bedeschi, F and Bisello, D and Blusk, S and Caskey, W and Chiarelli, G and Connolly, A and Demina, R and Ely, R and Field, R and Garcia-Sciveres, M and Giolo, K and Goldstein, D and Goldstein, J and Grim, G and Guerzoni, M and Haas, R and Haber, C and Hara, K and Hartmann, F and Heiss, A and Hill, C and Hrycyk,
M and Incandela, J and Kato, Y and Knoblauch, D and Kruse, M and Lander, R and Lei, CM and Leonardi, G and Leone, S and Martignon, G and Miyazaky, Y and Moggi, A and Muller, T and Munar, A and Okusawa, T and Palmonari, F and Paulini, M and Pellett, D and Piacentino, G and Raffaelli, F and Roederer, F and Saltzberg, D and Schilling, M and Shimojima, M and Stuart, D and Takano, T and Takikawa, K and Tanaka, M and Tipton, P and Turini, N and Volobouev, I and Yao, W and Yoshida, T and Wenzel, H and Wilkes, T and Zetti, F and Zucchelli, S},
Title = {The CDF intermediate silicon layers detector},
Journal = {Nuovo Cimento della Societa Italiana di Fisica
A},
Volume = {112},
Number = {11},
Pages = {1351-1357},
Year = {1999},
Month = {November},
Key = {fds308818}
}
@article{fds308744,
Author = {Aoki, M and Bacchetta, N and Behari, S and Benjamin, D and Bisello, D and Bolla, G and Bortoletto, D and Burghard, A and Busetto, G and Cabrera,
S and Canepa, A and Castro, A and Cardoso, G and Chertok, M and Ciobanu, C and Derylo, G and Fang, I and Flaugher, B and Freeman, J and Galtieri, L and Galyardt, J and Garcia-Sciveres, M and Giurgiu, G and Gorelov, I and Haber, C and Hara, K and Hoeferkamp, M and Holbrook, B and Hrycyk, M and Junk, T and Kim, S and Kobayashi, K and Krieger, B and Kruse, M and Lander,
R and Lu, RS and Lukens, P and Malferrari, L and Manea, C and Margotti, A and Maksimovic, P and Merkel, P and Moccia, S and Nakano, I and Naoumov, D and Novak, J and Okusawa, T and Orlov, Y and Pancaldi, G and Pantano, D and Pavlicek, V and Pellett, D and Seidel, S and Semeria, F and Takei, Y and Tanaka, R and Wang, Z and Watje, P and Weber, M and Wester, W and Wilkes,
T and Yamamoto, K and Yao, W and Zimmermann, S and Zucchelli, S and Zucchini, A},
Title = {The CDF Run IIb silicon detector},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {518},
Number = {1-2},
Pages = {270-276},
Publisher = {Elsevier BV},
Year = {2004},
Month = {February},
url = {http://dx.doi.org/10.1016/j.nima.2003.10.080},
Abstract = {Fermilab plans to deliver 5-15fb-1 of integrated luminosity
to the CDF and D0 experiments. The current inner silicon
detectors at CDF (SVXIIa and L00) will not tolerate the
radiation dose associated with high-luminosity running and
will need to be replaced. A new readout chip (SVX4) has been
designed in radiation-hard 0.25μm, CMOS technology.
Single-sided sensors are arranged in a compact structure,
called a stave, with integrated readout and cooling systems.
This paper describes the general design of the Run IIb
system, testing results of prototype electrical components
(staves), and prototype silicon sensor performance before
and after irradiation. © 2003 Elsevier B.V. All rights
reserved.},
Doi = {10.1016/j.nima.2003.10.080},
Key = {fds308744}
}
@article{fds308699,
Author = {Akimoto, T and Aoki, M and Azzi, P and Bacchetta, N and Behari, S and Benjamin, D and Bisello, D and Bolla, G and Bortoletto, D and Burghard,
A and Busetto, G and Cabrera, S and Canepa, A and Cardoso, G and Chertok,
M and Ciobanu, CI and Derylo, G and Fang, I and Feng, EJ and Fernandez, JP and Flaugher, B and Freeman, J and Galtieri, L and Galyardt, J and Garcia-Sciveres, M and Giurgiu, G and Gorelov, I and Haber, C and Hale,
D and Hara, K and Harr, R and Hill, C and Hoeferkamp, M and Hoff, J and Holbrook, B and Hong, SC and Hrycyk, M and Hsiung, TH and Incandela, J and Jeon, EJ and Joo, KK and Junk, T and Kahkola, H and Karjalainen, S and Kim,
S and Kobayashi, K and Kong, DJ and Krieger, B and Kruse, M and Kuznetsova,
N and Kyre, S and Lander, R and Landry, T and Lauhakangas, R and Lee, J and Lu, RS and Lujan, P and Lukens, P and Mandelli, E and Manea, C and Maksimovic, P and Merkel, P and Min, SN and Moccia, S and Nakano, I and Naoumov, D and Nelson, T and Nord, B and Novak, J and Okusawa, T and Orava,
R and Orlov, Y and Osterberg, K and Pantano, D and Pavlicek, V and Pellett,
D and Pursley, J and Riipinen, P and Schuyler, B and Seidel, S and Shenai,
A and Soha, A and Stuart, D and Tanaka, R and Tavi, M and Von Der Lippe and H and Walder, JP and Wang, Z and Watje, P and Weber, M and Wester, W and Yamamoto, K and Yang, YC and Yao, W and Yarema, R and Yun, JC and Zetti, F and Zimmerman, T},
Title = {The CDF Run IIb Silicon Detector: Design, preproduction, and
performance},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {556},
Number = {2},
Pages = {459-481},
Publisher = {Elsevier BV},
Year = {2006},
Month = {January},
url = {http://dx.doi.org/10.1016/j.nima.2005.11.046},
Abstract = {A new silicon microstrip detector was designed by the CDF
collaboration for the proposed high-luminosity operation of
the Tevatron pp̄ collider (Run IIb). The detector is
radiation-tolerant and will still be functional after
exposure to particle fluences of 10141-MeV equivalent
neutrons/cm2 and radiation doses of 20 MRad. The detector
will maintain or exceed the performance of the current CDF
silicon detector throughout Run IIb. It is based on an
innovative silicon "supermodule" design. Critical detector
components like the custom radiation-hard SVX4 readout chip,
the beryllia hybrids and mini-port (repeater) cards, and the
silicon sensors fulfill their specifications and were
produced with high yields. The design goals and solutions of
the CDF Run IIb silicon detector are described, and the
performance of preproduction modules is presented in detail.
Results relevant for the development of future silicon
systems are emphasized. Crown Copyright © 2005 Published by
Elsevier B.V. All rights reserved.},
Doi = {10.1016/j.nima.2005.11.046},
Key = {fds308699}
}
@article{fds321357,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M},
Title = {The differential production cross section of the [Formula:
see text](1020) meson in [Formula: see text] = 7 TeV
[Formula: see text] collisions measured with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {7},
Pages = {2895},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-2895-2},
Abstract = {A measurement is presented of the [Formula: see text]
production cross section at [Formula: see text] = 7 TeV
using [Formula: see text] collision data corresponding to an
integrated luminosity of 383 [Formula: see text], collected
with the ATLAS experiment at the LHC. Selection of [Formula:
see text](1020) mesons is based on the identification of
charged kaons by their energy loss in the pixel detector.
The differential cross section is measured as a function of
the transverse momentum, [Formula: see text], and rapidity,
[Formula: see text], of the [Formula: see text](1020) meson
in the fiducial region 500 [Formula: see text] 1200 MeV,
[Formula: see text] 0.8, kaon [Formula: see text] 230 MeV
and kaon momentum [Formula: see text] 800 MeV. The
integrated [Formula: see text]-meson production cross
section in this fiducial range is measured to be [Formula:
see text] = 570 [Formula: see text] 8 (stat) [Formula: see
text] 66 (syst) [Formula: see text] 20 (lumi) [Formula: see
text].},
Doi = {10.1140/epjc/s10052-014-2895-2},
Key = {fds321357}
}
@article{fds308819,
Author = {Affolder, A and Azzi-Bacchetta, P and Bacchetta, N and Barbaro-Galtieri, A and Basti, A and Bedeschi, F and Bisello, D and Blusk, S and Chertok, M and Chiarelli, G and Connolly, A and Demina, R and Donati, S and Ely, R and Field, R and Garcia-Sciveres, M and Goldstein,
J and Grim, G and Guerzoni, M and Haber, C and Hara, K and Hartmann, F and Heiss, A and Hill, C and Hrycyk, M and Incandela, J and Kato, Y and Kim,
BJ and Knoblauch, D and Kruse, M and Lei, M and Leone, S and Martignon, G and Mcyntire, P and Miyazaki, Y and Moggi, A and Muller, T and Munar-Ara, A and Okusawa, T and Palmonari, F and Paulini, M and Pellett, D and Piacentino, G and Raffaelli, F and Saltzberg, D and Sanders, E and Schilling, M and Shimojima, M and Stuart, D and Takano, T and Takikawa,
K and Tipton, P and Turini, N and Volobouev, I and Wenzel, H and Yao, W and Yoshida, T and Zetti, F and Zucchelli, S},
Title = {The intermediate silicon layers detector at CDFII: Design
and progress},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {435},
Number = {1-2},
Pages = {44-50},
Publisher = {Elsevier BV},
Year = {1999},
Month = {October},
url = {http://dx.doi.org/10.1016/S0168-9002(99)00408-8},
Abstract = {The Intermediate Silicon Layers Detector is presently being
built as part of the CDF upgrades to prepare for the next
Tevatron data taking run, scheduled to start in the year
2000. The ISL will be located in the radial region between
the Silicon Vertex Detector and the Central Outer Tracker.
It will add tracking in the forward region and significantly
improve tracking in the central region. Together with the
SVX II, the ISL forms a standalone, 3D silicon tracker. In
this article we present the design of the ISL and the
current status of its construction. © 1999 Elsevier Science
B.V. All rights reserved.},
Doi = {10.1016/S0168-9002(99)00408-8},
Key = {fds308819}
}
@article{fds321155,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner,
M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji,
W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito,
L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {The performance of the jet trigger for the ATLAS detector
during 2011 data taking.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {10},
Pages = {526},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4325-0},
Abstract = {The performance of the jet trigger for the ATLAS detector at
the LHC during the 2011 data taking period is described.
During 2011 the LHC provided proton-proton collisions with a
centre-of-mass energy of 7 TeV and heavy ion collisions
with a 2.76 TeV per nucleon-nucleon collision energy. The
ATLAS trigger is a three level system designed to reduce the
rate of events from the 40 MHz nominal maximum bunch
crossing rate to the approximate 400 Hz which can be
written to offline storage. The ATLAS jet trigger is the
primary means for the online selection of events containing
jets. Events are accepted by the trigger if they contain one
or more jets above some transverse energy threshold. During
2011 data taking the jet trigger was fully efficient for
jets with transverse energy above 25 GeV for triggers
seeded randomly at Level 1. For triggers which require a jet
to be identified at each of the three trigger levels, full
efficiency is reached for offline jets with transverse
energy above 60 GeV. Jets reconstructed in the final
trigger level and corresponding to offline jets with
transverse energy greater than 60 GeV, are reconstructed
with a resolution in transverse energy with respect to
offline jets, of better than 4 % in the central region and
better than 2.5 % in the forward direction.},
Doi = {10.1140/epjc/s10052-016-4325-0},
Key = {fds321155}
}
@article{fds308739,
Author = {al, DAE},
Title = {The Underlying event in hard interactions at the Fermilab
Tevatron p-barp collider},
Journal = {Physical Review},
Volume = {D70},
Number = {7},
Pages = {072002},
Publisher = {American Physical Society (APS)},
Year = {2004},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.70.072002},
Abstract = {For comparison of inclusive jet cross sections measured at
hadron-hadron colliders to next-to-leading order (NLO)
parton-level calculations, the energy deposited in the jet
cone by spectator parton interactions must first be
subtracted. The assumption made at the Tevatron is that the
spectator parton interaction energy is similar to the
ambient level measured in minimum bias events. In this
paper, we test this assumption by measuring the ambient
charged track momentum in events containing large transverse
energy jets at sqrt[s]=1800 GeV and sqrt[s]=630 GeV and
comparing this ambient momentum with that observed both in
minimum bias events and with that predicted by two Monte
Carlo models. Two cones in eta - phi space are defined, at
the same pseudorapidity, eta , as the jet with the highest
transverse energy (E(1)T), and at ±90o in the azimuthal
direction, phi . The total charged track momentum inside
each of the two cones is measured. The minimum momentum in
the two cones is almost independent of E(1)T and is similar
to the momentum observed in minimum bias events, whereas the
maximum momentum increases roughly linearly with the jet
E(1)T over most of the measured range. This study was
carried out using data from the CDF detector taken during
Run 1 (1994-1995). The study will help improve the precision
of comparisons of jet cross section data and NLO
perturbative QCD predictions. The distribution of the sum of
the track momenta in the two cones is also examined for five
different E(1)T bins. The HERWIG and PYTHIA Monte Carlo
generators are reasonably successful in describing the data,
but neither can describe completely all of the event
properties.},
Doi = {10.1103/PhysRevD.70.072002},
Key = {fds308739}
}
@article{fds308868,
Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas,
A and Berge, JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner,
N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao,
HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cronin-Hennessy, D and Culbertson,
R and Daniels, T and De Jongh and F and Delchamps, S and Dell’agnello, S and Dell’orso, M and Demina, R and Demortier, L},
Title = {The μτ and eτ decays of top quark pairs produced in pp¯
collisions at √s=1.8TeV},
Journal = {Physical Review Letters},
Volume = {79},
Number = {19},
Pages = {3585-3590},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.3585},
Abstract = {We present a search for dilepton events from tt¯ production
with one electron or muon and one hadronically decaying τ
lepton from the decay tt¯→(ℓνℓ)(τντ)bbú,
(ℓ=e,μ), using the Collider Detector at Fermilab. In a
109pb−1 data sample of pp¯ collisions at √S=1.8TeV we
expect ∼1 signal event and a total background of ∼2
events; we observe 4 candidate events (2eτ and 2μτ).
Three of these events have jets identified as b candidates,
compared to an estimated background of 0.28±0.02 events. ©
1997 The American Physical Society.},
Doi = {10.1103/PhysRevLett.79.3585},
Key = {fds308868}
}
@article{fds375896,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Tools for estimating fake/non-prompt lepton backgrounds with
the ATLAS detector at the LHC},
Journal = {Journal of Instrumentation},
Volume = {18},
Number = {11},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1088/1748-0221/18/11/T11004},
Abstract = {Measurements and searches performed with the ATLAS detector
at the CERN LHC often involve signatures with one or more
prompt leptons. Such analyses are subject to
'fake/non-prompt' lepton backgrounds, where either a hadron
or a lepton from a hadron decay or an electron from a photon
conversion satisfies the prompt-lepton selection criteria.
These backgrounds often arise within a hadronic jet because
of particle decays in the showering process, particle
misidentification or particle interactions with the detector
material. As it is challenging to model these processes with
high accuracy in simulation, their estimation typically uses
data-driven methods. Three methods for carrying out this
estimation are described, along with their implementation in
ATLAS and their performance.},
Doi = {10.1088/1748-0221/18/11/T11004},
Key = {fds375896}
}
@article{fds30250,
Author = {M.C. Kruse},
Title = {Top and Electroweak Physics from the Tevatron.},
Year = {2003},
Month = {October},
url = {http://arXiv.org/ps/hep-ex/0310057},
Abstract = {http://arXiv.org/abs/hep-ex/0310057},
Key = {fds30250}
}
@article{fds308667,
Author = {Abulencia, and A, and others},
Title = {Top quark mass measurement from dilepton events at CDF
II},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {15},
Pages = {152002},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.152002},
Abstract = {We report a measurement of the top quark mass using events
collected by the CDF II Detector from p anti-p collisions at
s**(1/2) = 1.96 TeV at the Fermilab Tevatron. We calculate a
likelihood function for the top mass in events that are
consistent with t anti-t --> b-bar l- nu-bar_l bl'+ nu'_l
decays. The likelihood is formed as the convolution of the
leading-order matrix element and detector resolution
functions. The joint likelihood is the product of
likelihoods for each of 33 events collected in 340 pb-1 of
integrated luminosity, yielding a top quark mass M_t = 165.2
+/- 6.1(stat.) +/- 3.4(syst.) GeV/c2. This first application
of a matrix-element technique to tt-bar --> bl+ nu_l b-bar
l'- nu-bar_l' decays gives the most precise single
measurement of M_t in dilepton events. Combined with other
CDF Run II measurements using dilepton events, we measure
M_t = 167.9 +/- 5.2(stat.) +/- 3.7(syst.)
GeV/c2.},
Doi = {10.1103/physrevlett.96.152002},
Key = {fds308667}
}
@article{fds308689,
Author = {Abulencia, and A, and others},
Title = {Top quark mass measurement from dilepton events at CDF II
with the matrix-element method},
Journal = {Phys. Rev.},
Volume = {D74},
Number = {3},
Pages = {032009},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.74.032009},
Abstract = {We describe a measurement of the top quark mass using events
with two charmed leptons collected by the CDF II detector
from p anti-p collisions with s**(1/2) = 1.96 TeV at the
Fermilab Tevatron. The likelihood in top mass is calculated
for each event by convoluting the leading order matrix
element describing qqbar --> t anti-t --> b l nu_l b-bar l'
nu_l' with detector resolution functions. The presence of
background events in the data sample is modeled using
similar calculations involving the matrix elements for major
background processes. In a data sample with integrated
luminosity of 340 pb-1, we observe 33 candidate events and
measure M_top = 165.2 +/- 6.1(stat.) +/- 3.4(syst.) GeV/c2.
This measurement represents the first application of this
method to events with two charged leptons and is the most
precise single measurement of the top quark mass in this
channel.},
Doi = {10.1103/PhysRevD.74.032009},
Key = {fds308689}
}
@article{fds308468,
Author = {Aaltonen, and T, and others},
Title = {Top Quark Mass Measurement in the $lepton+jets$ Channel
Using a Matrix Element Method and in situ Jet Energy
Calibration},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {25},
Pages = {252001},
Publisher = {American Physical Society},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.252001},
Abstract = {A precision measurement of the top quark mass m(t) is
obtained using a sample of tt events from pp collisions at
the Fermilab Tevatron with the CDF II detector. Selected
events require an electron or muon, large missing transverse
energy, and exactly four high-energy jets, at least one of
which is tagged as coming from a b quark. A likelihood is
calculated using a matrix element method with quasi-Monte
Carlo integration taking into account finite detector
resolution and jet mass effects. The event likelihood is a
function of m(t) and a parameter Δ(JES) used to calibrate
the jet energy scale in situ. Using a total of 1087 events
in 5.6 fb(-1) of integrated luminosity, a value of
m(t)=173.0 ± 1.2 GeV/c(2) is measured.},
Doi = {10.1103/PhysRevLett.105.252001},
Key = {fds308468}
}
@article{fds308552,
Author = {Aaltonen, T and others},
Title = {Top quark mass measurement in the lepton plus jets channel
using a modified matrix element method},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {7},
Pages = {072001},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.072001},
Abstract = {We report a measurement of the top quark mass, mt, obtained
from pp̄ collisions at s=1.96TeV at the Fermilab Tevatron
using the CDF II detector. We analyze a sample corresponding
to an integrated luminosity of 1.9fb-1. We select events
with an electron or muon, large missing transverse energy,
and exactly four high-energy jets in the central region of
the detector, at least one of which is tagged as coming from
a b quark. We calculate a signal likelihood using a matrix
element integration method, where the matrix element is
modified by using effective propagators to take into account
assumptions on event kinematics. Our event likelihood is a
function of mt and a parameter JES (jet energy scale) that
determines in situ the calibration of the jet energies. We
use a neural network discriminant to distinguish signal from
background events. We also apply a cut on the peak value of
each event likelihood curve to reduce the contribution of
background and badly reconstructed events. Using the 318
events that pass all selection criteria, we find
mt=172.7±1.8(stat+JES) ±1.2(syst)GeV/c2. © 2009 The
American Physical Society.},
Doi = {10.1103/PhysRevD.79.072001},
Key = {fds308552}
}
@article{fds308551,
Author = {Aaltonen, T and others},
Title = {Top quark mass measurement in the tt̅ all hadronic channel
using a matrix element technique in pp̅ collisions at
sqrt[s] =1.96 TeV},
Journal = {Physical Review D},
Volume = {79},
Number = {7},
Pages = {072010},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.072010},
Abstract = {We present a measurement of the top quark mass in the all
hadronic channel (tt̅ →bb̅ q1q̅ 2q3q̅ 4) using
943 pb-1 of pp̅ collisions at sqrt[s]=1.96 TeV
collected at the CDF II detector at Fermilab (CDF). We apply
the standard model production and decay matrix element (ME)
to tt̅ candidate events. We calculate per-event probability
densities according to the ME calculation and construct
template models of signal and background. The scale of the
jet energy is calibrated using additional templates formed
with the invariant mass of pairs of jets. These templates
form an overall likelihood function that depends on the top
quark mass and on the jet energy scale (JES). We estimate
both by maximizing this function. Given 72 observed events,
we measure a top quark mass of 171.1 ± 3.7(stat+JES)
± 2.1(syst) GeV/c2. The combined uncertainty on
the top quark mass is 4.3 GeV/c2.},
Doi = {10.1103/PhysRevD.79.072010},
Key = {fds308551}
}
@article{fds308499,
Author = {Aaltonen, and T, and others},
Title = {Top Quark Mass Measurement using $m_{T2}$ in the Dilepton
Channel at CDF},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {3},
Pages = {031102},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.031102},
Abstract = {http://arxiv.org/abs/0911.2956},
Doi = {10.1103/PhysRevD.81.031102},
Key = {fds308499}
}
@article{fds308445,
Author = {Aaltonen, and T, and al, E},
Title = {Top quark mass measurement using the template method at
{CDF}},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {11},
Pages = {111101},
Publisher = {American Physical Society},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.83.111101},
Abstract = {We present a measurement of the top quark mass in the
lepton+jets and dilepton channels of tt̄ decays using the
data sample corresponding to an integrated luminosity of
5.6fb-1 of pp̄ collisions at Tevatron with √s=1.96TeV,
collected with the CDF II detector. We construct templates
of two reconstructed top quark masses from different
jets-to-quarks combinations and the invariant mass of two
jets from the W decays in the lepton+jets channel, and a
reconstructed top quark mass and mT2, a variable related to
the transverse mass in events with two missing particles, in
the dilepton channel. The simultaneous fit of the templates
from signal and background events in the lepton+jets and
dilepton channels to the data yields a measured top quark
mass of Mtop=172.1±1.1(stat)±0. 9(syst)GeV/c2. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.83.111101},
Key = {fds308445}
}
@article{fds308675,
Author = {Abulencia, and A, and others},
Title = {Top quark mass measurement using the template method in the
lepton + jets channel at CDF II},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {3},
Pages = {032003},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.73.032003},
Abstract = {This article presents a measurement of the top quark mass
using the CDF II detector at Fermilab. Colliding beams of
protons and anti-protons at Fermilab's Tevatron (s**(1/2) =
1.96 TeV) produce top/anti-top pairs, which decay to W+ W-
bb-bar; events are selected where one W decays to hadrons,
and the other W decays to either e or mu plus a neutrino.
The data sample corresponds to an integrated luminosity of
approximately 318 pb-1. A total of 165 tt-bar events are
separated into four subsamples based on jet transverse
energy thresholds and the number of b jets identified by
reconstructing a displaced vertex. In each event, the
reconstructed top quark invariant mass is determined by
minimizing a chi2 for the overconstrained kinematic system.
At the same time, the mass of the hadronically decaying W
boson is measured in the same event sample. The observed W
boson mass provides an in situ improvement in the
determination of the hadronic jet energy scale, JES. A
simultaneous likelihood fit of the reconstructed top quark
masses and the W boson invariant masses in the data sample
to distributions from simulated signal and background events
gives a top quark mass of 173.5+3.7_-3.6(stat. + JES) +/-
1.3 (other syst.) GeV/c2, or 173.5+3.9_-3.8
GeV/c2.},
Doi = {10.1103/PhysRevD.73.032003},
Key = {fds308675}
}
@article{fds308324,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Top-quark mass measurement in events with jets and missing
transverse energy using the full CDF data
set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.88.011101},
Abstract = {We present a measurement of the top-quark mass using the
full data set of Tevatron √s=1.96 TeV proton-antiproton
collisions recorded by the CDF II detector, corresponding to
an integrated luminosity of 8.7 fb-1. The analysis uses
events with one semileptonic t or t̄ decay, but without
detection of the electron or muon. We select events with
significant missing transverse energy and multiple jets. We
veto events containing identified electrons or muons. We
obtain distributions of the top-quark masses and the
invariant mass of the two jets from W-boson decays from data
and compare these to templates derived from signal and
background samples to extract the top-quark mass and the
energy scale of the calorimeter jets with in situ
calibration. A likelihood fit of the templates from signal
and background events to the data yields the top-quark mass,
Mtop=173.93±1.64(stat)±0. 87(syst) GeV/c2. This result is
the most precise measurement to date of the mass of the top
quark in this event topology. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.011101},
Key = {fds308324}
}
@article{fds308425,
Author = {Aaltonen, TEA},
Title = {Top-Quark Mass Measurement Using Events with Missing
Transverse Energy and Jets at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {23},
Pages = {232002},
Publisher = {American Physical Society},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.232002},
Abstract = {We present a measurement of the top-quark mass using a
sample of $t\bar{t}$ events in 5.7 fb-1 of integrated
luminosity from $p\bar{p}$ collisions at the Fermilab
Tevatron with $\sqrt{s}=1.96$ TeV and collected by the
CDF II Detector. We select events having large missing
transverse energy, and four, five, or six jets with at least
one jet tagged as coming from a b quark, and reject events
with identified charged leptons. This analysis considers
events from the semileptonic tt̅ decay channel, including
events that contain tau leptons. The measurement is based on
a multidimensional template method. We fit the data to
signal templates of varying top-quark masses and background
templates, and measure a top-quark mass of Mtop=$172.32\pm
2.4$(stat)$\pm 1.0$(syst) GeV/c2.},
Doi = {10.1103/PhysRevLett.107.232002},
Key = {fds308425}
}
@article{fds308805,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Antos, J and Apollinari, G and Arisawa,
T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge,
JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker,
C and Bloom, K and Blusk, S and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl,
A and Brink, SVD and Bromberg, C and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlson,
J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng,
MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze,
G and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Cobal, M and Cocca, E and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Costa, JGD and Costanzo, D and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Erdmann, W and Errede, D and Errede, S and Fan,
Q and Feild, RG and Ferretti, C and Fiori, I and Flaugher, B and Foster,
GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer,
S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold,
M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos,
K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Guo, RS and Haber, C and Hafen, E and Hahn,
SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama,
K and Hauser, J and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman,
KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston,
J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov,
A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and Lee,
AM and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Meschi, E and Mesropian, C and Miao, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Moggi, N and Moore, E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman, J and Nahn,
S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti,
R and Papadimitriou, V and Pappas, SP and Parri, A and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos,
A and Pondrom, L and Pope, G and Prokoshin, F and Proudfoot, J and Ptohos,
F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takashima, R and Takikawa, K and Tanaka, M and Takano, T and Tannenbaum,
B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Ukegawa, F and Valls, J and Vejcik, S and Velev, G and Vidal, R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Transverse Momentum and Total Cross Section of
e+e- Pairs in the Z-Boson Region from
pp̄ Collisions at √s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {84},
Number = {5},
Pages = {845-850},
Year = {2000},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.84.845},
Abstract = {The transverse momentum and total cross section of e+e−
pairs in the Z-boson region of 66<Mee<116GeV/c2 from pp¯
collisions at √s=1.8TeV are measured using 110 pb−1 of
collisions taken by the Collider Detector at Fermilab during
1992-1995. The total cross section is measured to be 248±11
pb. The differential transverse momentum cross section is
compared with calculations that match quantum chromodynamics
perturbation theory at high transverse momentum with the
gluon resummation formalism at low transverse momentum. ©
2000 The American Physical Society.},
Doi = {10.1103/PhysRevLett.84.845},
Key = {fds308805}
}
@article{fds308408,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Transverse momentum cross section of e +e
- pairs in the Z-boson region from pp̄
collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.86.052010},
Abstract = {The transverse momentum cross section of e +e - pairs in the
Z-boson mass region of 66-116GeV/c2 is precisely measured
using Run II data corresponding to 2.1fb -1 of integrated
luminosity recorded by the Collider Detector at Fermilab.
The cross section is compared with two quantum chromodynamic
calculations. One is a fixed-order perturbative calculation
at O(αs2), and the other combines perturbative predictions
at high transverse momentum with the gluon resummation
formalism at low transverse momentum. Comparisons of the
measurement with calculations show reasonable agreement. The
measurement is of sufficient precision to allow refinements
in the understanding of the transverse momentum
distribution. © 2012 American Physical Society.},
Doi = {10.1103/PhysRevD.86.052010},
Key = {fds308408}
}
@article{fds321144,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
A},
Title = {Transverse momentum, rapidity, and centrality dependence of
inclusive charged-particle production in sNN=5.02
TeV p + Pb collisions measured by the ATLAS
experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {763},
Pages = {313-336},
Publisher = {Elsevier BV},
Year = {2016},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2016.10.053},
Abstract = {Measurements of the per-event charged-particle yield as a
function of the charged-particle transverse momentum and
rapidity are performed using p+Pb collision data collected
by the ATLAS experiment at the LHC at a centre-of-mass
energy of sNN=5.02TeV. Charged particles are reconstructed
over pseudorapidity |η|<2.3 and transverse momentum between
0.1 GeV and 22 GeV in a dataset corresponding to an
integrated luminosity of 1 μb−1. The results are
presented in the form of charged-particle nuclear
modification factors, where the p+Pb charged-particle
multiplicities are compared between central and peripheral
p+Pb collisions as well as to charged-particle cross
sections measured in pp collisions. The p+Pb collision
centrality is characterized by the total transverse energy
measured in −4.9<η<−3.1, which is in the direction of
the outgoing lead beam. Three different estimations of the
number of nucleons participating in the p+Pb collision are
carried out using the Glauber model and two Glauber–Gribov
colour-fluctuation extensions to the Glauber model. The
values of the nuclear modification factors are found to vary
significantly as a function of rapidity and transverse
momentum. A broad peak is observed for all centralities and
rapidities in the nuclear modification factors for
charged-particle transverse momentum values around 3 GeV.
The magnitude of the peak increases for more central
collisions as well as rapidity ranges closer to the
direction of the outgoing lead nucleus.},
Doi = {10.1016/j.physletb.2016.10.053},
Key = {fds321144}
}
@article{fds365353,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Two-particle Bose–Einstein correlations in pp collisions
at √s=13 TeV measured with the ATLAS detector at the
LHC},
Journal = {European Physical Journal C},
Volume = {82},
Number = {7},
Year = {2022},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10472-0},
Abstract = {This paper presents studies of Bose–Einstein correlations
(BEC) in proton–proton collisions at a centre-of-mass
energy of 13 TeV, using data from the ATLAS detector at the
CERN Large Hadron Collider. Data were collected in a special
low-luminosity configuration with a minimum-bias trigger and
a high-multiplicity track trigger, accumulating integrated
luminosities of 151 μ b- 1 and 8.4 nb- 1, respectively.
The BEC are measured for pairs of like-sign charged
particles, each with | η| < 2.5 , for two kinematic ranges:
the first with particle pT> 100 MeV and the second with
particle pT> 500 MeV. The BEC parameters, characterizing the
source radius and particle correlation strength, are
investigated as functions of charged-particle multiplicity
(up to 300) and average transverse momentum of the pair (up
to 1.5 GeV). The double-differential dependence on
charged-particle multiplicity and average transverse
momentum of the pair is also studied. The BEC radius is
found to be independent of the charged-particle multiplicity
for high charged-particle multiplicity (above 100),
confirming a previous observation at lower energy. This
saturation occurs independent of the transverse momentum of
the pair.},
Doi = {10.1140/epjc/s10052-022-10472-0},
Key = {fds365353}
}
@article{fds308508,
Author = {Aaltonen, and T, and others},
Title = {Updated search for the flavor-changing neutral-current decay
$D^{0}\rightarrow{}\mu{}^{+}\mu{}^{-}$ in $pp[over
\ifmmode\bar\else\textasciimacron\fi{}]$ collisions at
$\sqrt{s}=1.96$ TeV},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {9},
Pages = {091105},
Publisher = {American Physical Society},
Year = {2010},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.82.091105},
Abstract = {We report on a search for the flavor-changing
neutral-current decay D0→μ⊃+μ⊃- in pp̄ collisions
at √s=1.96TeV using 360pb⊃-1 of integrated luminosity
collected by the CDF II detector at the Fermilab Tevatron
collider. A displaced vertex trigger selects long-lived D0
candidates in the μ⊃+μ⊃-, π⊃+π⊃-, and
K⊃-π⊃+ decay modes. We use the Cabibbo-favored
D0→K⊃- π⊃+ channel to optimize the selection criteria
in an unbiased manner, and the kinematically similar
D0→π⊃+π⊃- channel for normalization. We set an upper
limit on the branching fraction B(D0→μ⊃+μ⊃-)<2.1×10⊃-7(3.0×10⊃-7)
at the 90% (95%) confidence level. © 2010 The American
Physical Society.},
Doi = {10.1103/PhysRevD.82.091105},
Key = {fds308508}
}
@article{fds308354,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Updated search for the standard model Higgs boson in events
with jets and missing transverse energy using the full CDF
data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.87.052008},
Abstract = {We present an updated search for the Higgs boson produced in
association with a vector boson in the final state with
missing transverse energy and two jets. We use the full CDF
data set corresponding to an integrated luminosity of 9.45
fb-1 at a proton-antiproton center-of-mass energy of
√s=1.96 TeV. New to this analysis is the inclusion of a
b-jet identification algorithm specifically optimized for
H→bb̄ searches. Across the Higgs boson mass range
90≤mH≤150 GeV/c2, the expected 95% credibility level
upper limits on the VH production cross section times the
H→bb̄ branching fraction are improved by an average of
14% relative to the previous analysis. At a Higgs boson mass
of 125 GeV/c2, the observed (expected) limit is 3.06 (3.33)
times the standard model prediction, corresponding to one of
the most sensitive searches to date in this final state. ©
2013 American Physical Society.},
Doi = {10.1103/PhysRevD.87.052008},
Key = {fds308354}
}
@article{fds330933,
Author = {al, DAE},
Title = {Upsilon Production and Polarization in pp Collisions at
$\sqrt{s} = 1.8TeV},
Journal = {Physical Review Letters},
Volume = {88},
Number = {16},
Pages = {161802},
Year = {2002},
url = {http://dx.doi.org/10.1103/physrevlett.88.161802},
Abstract = {We report on measurements of the Upsilon(1S), Upsilon(2S),
and Upsilon(3S) differential cross sections
(d(2)sigma/dp(T)dy)(/y/<0.4), as well as on the Upsilon(1S)
polarization in p p macro collisions at square root of s =
1.8 TeV using a sample of 77+/-3 pb(-1) collected by the
collider detector at Fermilab. The three resonances were
reconstructed through the decay Upsilon-->mu(+)mu(-). The
measured angular distribution of the muons in the
Upsilon(1S) rest frame is consistent with unpolarized meson
production.},
Doi = {10.1103/physrevlett.88.161802},
Key = {fds330933}
}
@article{fds308918,
Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and al, E},
Title = {W Boson + Jet Angular distribution in pp̄ collsions at
s=1.8 TeV},
Journal = {Physical Review Letters},
Volume = {73},
Number = {17},
Pages = {2296-2300},
Year = {1994},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.73.2296},
Abstract = {The W+jet angular distribution is measured using W→eν
events recorded with the Collider Detector at Fermilab (CDF)
during the 1988-89 and 1992-93 Tevatron runs. The data agree
well with both a leading order and a next-to-leading order
theoretical prediction. The shape of the angular
distribution is similar to that observed in photon + jet
data and significantly different from that observed in dijet
data. © 1994 The American Physical Society.},
Doi = {10.1103/PhysRevLett.73.2296},
Key = {fds308918}
}
@article{fds331627,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and D'Errico, M},
Title = {W-boson polarization measurement in the tt- dilepton channel
using the CDF II detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {722},
Number = {1-3},
Pages = {48-54},
Publisher = {Elsevier BV},
Year = {2013},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2013.03.032},
Abstract = {We present a measurement of the W-boson polarization in
top-quark decays in tt- events with decays to dilepton final
states using data corresponding to 5.1 fb-1 of integrated
luminosity in pp- collisions collected by the CDF II
detector at the Tevatron. Assuming a top-quark mass of 172.5
GeV/c2, a simultaneous measurement of the fractions of
longitudinal ( f0) and right-handed ( f+) W-bosons yields
the results f0 = 0.70-0.17+0.18 (stat) ± 0.06(syst) and f+
=-0.09 ± 0.09(stat) ± 0.03(syst). Combining this
measurement with our previous measurement based on
single-lepton final states, we obtain f0 = 0.84 ±
0.09(stat) ± 0.05(syst) and f+ =-0.16 ± 0.05(stat) ±
0.04(syst). The results are consistent with the standard
model expectation.},
Doi = {10.1016/j.physletb.2013.03.032},
Key = {fds331627}
}
@article{fds323772,
Author = {al, TAE},
Title = {``A Measurement of the Differential Dijet Mass Cross Section
in $p\overline p$ Collisions at $\sqrt{s} = 1.8$
TeV,''},
Journal = {Physical Review},
Volume = {D61},
Number = {9},
Pages = {091101},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevD.61.091101},
Abstract = {We present a measurement of the cross section for production
of two or more jets as a function of dijet mass, based on an
integrated luminosity of 86 (Formula presented) collected
with the Collider Detector at Fermilab. Our dijet mass
spectrum is described within errors by next-to-leading order
QCD predictions using CTEQ4HJ parton distributions, and is
in good agreement with a similar measurement from the DØ
experiment. © 2000 The American Physical
Society.},
Doi = {10.1103/PhysRevD.61.091101},
Key = {fds323772}
}
@article{fds331634,
Author = {al, DAE},
Title = {``Branching ratio measurements of exclusive B+ decays to
charmonium with the Collider Detector at
Fermilab},
Journal = {Physical Review},
Volume = {D66},
Number = {66},
Pages = {052005},
Publisher = {American Physical Society (APS)},
Year = {2002},
url = {http://dx.doi.org/10.1103/PhysRevD.66.052005},
Abstract = {We report on measurements of the branching ratios of the
decays B+ →(Formula presented)(1P)K+ and
B+→J/ψK+π+π-, where (Formula presented) (1P)→J/ψγ
and J/ψ→μ+μ- in pp collisions at (Formula presented)1.8
TeV. Using a data sample from an integrated luminosity of
110 pb-1 collected by the Collider Detector at Fermilab we
measure the branching ratios to be BR(B+→(Formula
presented) (1P)K+)=15.5±5.4(stat)±1.5(syst)±1.3(br)×10-4
and BR(B+→J/ψK+π+π-)=6.9±1.8(stat)±1.1(syst)±0.4(br)×10-4
where (br) is due to the finite precision on
BR(B+→J/ψK+), BR(Formula presented)(1P)→J/ψγ) is used
to normalize the signal yield, and (syst) encompasses all
other systematic uncertainties.},
Doi = {10.1103/PhysRevD.66.052005},
Key = {fds331634}
}
@article{fds331633,
Author = {al, DAE},
Title = {``Cross section for forward J/$ production in pp collisions
at $\sqrt{s} = 1.8 TeV,''},
Journal = {Physical Review},
Volume = {D66},
Number = {9},
Pages = {092001},
Publisher = {American Physical Society (APS)},
Year = {2002},
url = {http://dx.doi.org/10.1103/PhysRevD.66.092001},
Abstract = {The inclusive cross section for [Formula Presented]
production times the branching ratio [Formula Presented] has
been measured in the forward pseudorapidity region: [Formula
Presented] The results are based on [Formula Presented] of
data collected by the CDF Collaboration at the Fermilab
Tevatron Collider. The measurements extend earlier
measurements of the D0 Collaboration to higher [Formula
Presented] In the kinematic range where the experiments
partially overlap, these data are in good agreement with
previous measurements. © 2002 The American Physical
Society.},
Doi = {10.1103/PhysRevD.66.092001},
Key = {fds331633}
}
@article{fds331643,
Author = {al, TAE},
Title = {``Diffractive dijets with a leading antiproton in
$p\overline p$ Collisions at $\sqrt{s} = 1.8$
TeV,''},
Journal = {Physical Review Letters},
Volume = {84},
Number = {22},
Pages = {5043},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevLett.84.5043},
Abstract = {We report results from a study of events with a leading
antiproton of beam momentum fraction 0.905 < xF< 0.965 and
4-momentum transfer squared |t| < 3GeV2produced in ⊯pp
collisions at ⊡ s = 1800GeV at the Fermilab Tevatron
collider. Approximately 2% of the events contain two jets of
transverse energy EjetT> 7GeV. Using the dijet events, we
evaluate the diffractive structure function of the
antiproton and compare it with expectations based on results
obtained in diffractive deep inelastic scattering
experiments at the DESY ep collider HERA. © 2000 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.84.5043},
Key = {fds331643}
}
@article{fds308801,
Author = {al, TAE},
Title = {``Dijet production by double pomeron exchange at the
Fermilab Tevatron,''},
Journal = {Physical Review Letters},
Volume = {85},
Number = {20},
Pages = {4215},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevLett.85.4215},
Abstract = {Dijet production by double Pomeron exchange (DPE) in p̄p
collisions at √ s = 1800 GeV was performed. Factorization
was tested by comparing the diffractive structure function
measured in single diffractive (SD) with that determined
from DPE. As a result, a class of events with a double
Pomeron exchange topology were observed.},
Doi = {10.1103/PhysRevLett.85.4215},
Key = {fds308801}
}
@article{fds308590,
Author = {al, TAE},
Title = {``Direct measurement of the $W$ boson width in $p\overline
p$ Collisions at $\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review Letters},
Volume = {85},
Number = {7},
Pages = {3347},
Year = {2000},
url = {http://dx.doi.org/10.1103/physrevlett.100.071801},
Abstract = {A direct measurement of the total decay width of the W boson
Gamma(W) is presented using 350 pb(-1) of data from pp[over
] collisions at square root s = 1.96 TeV collected with the
CDF II detector at the Fermilab Tevatron. The width is
determined by normalizing predicted signal and background
distributions to 230 185 W candidates decaying to enu and
micronu in the transverse-mass region 50<M(T)<90 GeV and
then fitting the predicted shape to 6055 events in the
high-M(T) region, 90<M(T)<200 GeV. The result is
Gamma(W)=2032 +/- 45(stat)+/-57(syst) MeV, consistent with
the standard model expectation.},
Doi = {10.1103/physrevlett.100.071801},
Key = {fds308590}
}
@article{fds308772,
Author = {al, TAE},
Title = {``Double Diffraction Dissociation at the Fermilab Tevatron
Collider,''},
Journal = {Physical Review Letters},
Volume = {87},
Number = {14},
Pages = {141802},
Year = {2001},
url = {http://dx.doi.org/10.1103/physrevlett.87.141802},
Abstract = {We present results from a measurement of double diffraction
dissociation in pp collisions at the Fermilab Tevatron
collider. The production cross section for events with a
central pseudorapidity gap of width Deltaeta(0)>3
(overlapping eta = 0) is found to be 4.43+/-0.02(stat)+/-1.18(syst)
mb [ 3.42+/-0.01(stat)+/-1.09(syst) mb] at square root of
(s) = 1800[630] GeV. Our results are compared with previous
measurements and with predictions based on Regge theory and
factorization.},
Doi = {10.1103/physrevlett.87.141802},
Key = {fds308772}
}
@article{fds308775,
Author = {al, TAE},
Title = {``First Measurement of the Ratio $B(t \ra Wb)/B(t\ra Wq)$
and Associated Limit on the Cabibbo-Kobayashi-Maskawa
Element $|V_{tb}|$,''},
Journal = {Physical Review Letters},
Volume = {86},
Number = {15},
Pages = {3233},
Year = {2001},
url = {http://dx.doi.org/10.1103/physrevlett.86.3233},
Abstract = {We present the first measurement of the ratio of branching
fractions R identical withB(t-->Wb)/B(t-->Wq) from p_p
collisions at sqrt[s] = 1.8 TeV. The data set corresponds to
109 pb(-1) of data recorded by the Collider Detector at
Fermilab during the 1992-95 Tevatron run. We measure R =
0.94(+0.31)(-0.24)(stat+syst) or R>0.61 (0.56) at 90% (95)%
C.L., in agreement with the standard model predictions. This
measurement yields a limit on the Cabibbo-Kobayashi-Maskawa
quark mixing matrix element /V(tb)/ under the assumption of
three generations and unitarity.},
Doi = {10.1103/physrevlett.86.3233},
Key = {fds308775}
}
@article{fds308848,
Author = {al, FAE},
Title = {``Jet Pseudorapidity Distribution in Direct Photon Events in
$\overline pp$ Collisions at $\sqrt s$ =1.8
TeV,''},
Journal = {Physical Review},
Volume = {D57},
Number = {3},
Pages = {1359},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevD.57.1359},
Abstract = {We present the first measurement of the jet pseudorapidity
distribution in direct photon events from a sample of
(Formula presented) collisions at (Formula presented)
recorded with the Collider Detector at Fermilab. Quantum
chromodynamics (QCD) predicts that these events are
primarily from hard quark-gluon Compton scattering, (Formula
presented) with the final state quark producing the jet of
hadrons. The jet pseudorapidity distribution in this model
is sensitive to parton momentum fractions between 0.015 and
0.15. We find that the shape of the measured pseudorapidity
distribution agrees well with next-to-leading order QCD
calculations. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevD.57.1359},
Key = {fds308848}
}
@article{fds308799,
Author = {al, TAE},
Title = {``Limits on gravitino production and new processes with
large missing transverse energy in $p\overline p$ Collisions
at $\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review Letters},
Volume = {85},
Number = {7},
Pages = {1378},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevLett.85.1378},
Abstract = {Events collected by the Collider Detector at Fermilab (CDF)
with an energetic jet plus large missing transverse energy
can be used to search for physics beyond the standard model.
We see no deviations from the expected backgrounds and set
upper limits on the production of new processes. We consider
in addition the production of light gravitinos and set a
limit at 95% F ≥ 217GeV, which excludes gravitino masses
smaller than 1.1 × 10−5eV/c2. © 2000 American Physical
Society.},
Doi = {10.1103/PhysRevLett.85.1378},
Key = {fds308799}
}
@article{fds308823,
Author = {al, FAE},
Title = {``Measurement of $B$ Hadron Lifetimes Using J/$\psi$ final
States at CDF,''},
Journal = {Physical Review},
Volume = {D57},
Number = {9},
Pages = {5382},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevD.57.5382},
Abstract = {The average bottom-hadron and individual (Formula
presented), (Formula presented), and (Formula presented)
meson lifetimes have been determined using decays with a
(Formula presented) in the final state. The data sample
consists of 110 pb(Formula presented) of (Formula presented)
collisions at (Formula presented) TeV collected by the CDF
detector at the Fermilab Tevatron collider during
1992–1995. For the average lifetime of (Formula presented)
hadrons decaying into (Formula presented)+X, we obtain
(Formula presented) For the (Formula presented) and (Formula
presented) meson lifetimes, we determine (Formula presented)
(Formula presented) and (Formula presented) For the (Formula
presented) meson lifetime, we find (Formula presented) ps.
© 1998 The American Physical Society.},
Doi = {10.1103/PhysRevD.57.5382},
Key = {fds308823}
}
@article{fds323774,
Author = {al, FAE},
Title = {``Measurement of $b$ Quark Fragmentation Fractions in the
Production of Strange and Light $B$ Mesons in $p\overline p$
Collisions at $\sqrt{s} = 1.8$ TeV,"},
Journal = {Physical Review},
Volume = {D60},
Number = {9},
Pages = {092005},
Publisher = {American Physical Society (APS)},
Year = {1999},
url = {http://dx.doi.org/10.1103/PhysRevD.60.092005},
Abstract = {A new technique to measure the ratio of b quark
fragmentation fractions in (Formula presented) collisions is
described. Using a (Formula presented) sample of low-mass
dimuon trigger data recorded with the Collider Detector at
Fermilab, we identify B mesons by observing the double
semileptonic decays (Formula presented) with (Formula
presented) By counting the numbers of (Formula presented)
(Formula presented) and φ(1020) mesons produced in
association with these muon pairs, we measure the ratio of
strange to nonstrange B meson production to be (Formula
presented) This measurement is the most precise available
from hadron collisions to date. Limits on the branching
fractions of semileptonic charm meson decays with (Formula
presented) (Formula presented) and (Formula presented)
mesons in the final state are also obtained. © 1999 The
American Physical Society.},
Doi = {10.1103/PhysRevD.60.092005},
Key = {fds323774}
}
@article{fds308788,
Author = {al, TAE},
Title = {``Measurement of $b$-Quark Fragmentation Fractions in
$p\overline p$ Collisions at $\sqrt{s} = 1.8$
TeV,"},
Journal = {Physical Review Letters},
Volume = {84},
Number = {8},
Pages = {1663},
Year = {2000},
url = {http://dx.doi.org/10.1103/physrevlett.84.1663},
Abstract = {We have studied the production of B hadrons in 1.8-TeV
pp[over ¯] collisions. We present measurements of the
fragmentation fractions, f_{u}, f_{d}, f_{s}, and
f_{baryon}, of produced b quarks that yield B^{+}, B^{0},
B_{s}^{0}, and Λ[over ¯]_{b}^{0} hadrons. Reconstruction
of five electron-charm final states yields f_{s}/(
f_{u}+f_{d})=0.213±0.068 and f_{baryon}/(
f_{u}+f_{d})=0.118±0.042, assuming f_{u}=f_{d}. If all B
hadrons produced in pp[over ¯] collisions cascade to one of
these four hadrons, we determine f_{u}=f_{d}=0.375±0.023,
f_{s}=0.160±0.044, and f_{baryon}=0.090±0.029. If we do
not assume f_{u}=f_{d}, we find f_{d}/f_{u}=0.84±0.16.},
Doi = {10.1103/physrevlett.84.1663},
Key = {fds308788}
}
@article{fds314164,
Author = {al, FAE},
Title = {``Measurement of $B^0$-$\overline{B^0}$ Flavor Oscillations
using Jet-Charge and Lepton Flavor Tagging in $p\overline p$
Collisions at $\sqrt{s} = 1.8$ TeV,"},
Journal = {Physical Review},
Volume = {D60},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society (APS)},
Year = {1999},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.60.072003},
Abstract = {We present a measurement of the mass difference (Formula
presented) for the (Formula presented) meson and the
statistical power of the b flavor tagging methods used. The
measurement uses (Formula presented) of data from (Formula
presented) collisions at (Formula presented) collected with
the CDF detector. An inclusive lepton trigger is used to
collect a large sample of B hadron semileptonic decays. The
mass difference (Formula presented) is determined from the
proper time dependence of the fraction of B hadrons that
undergo flavor oscillations. The flavor at decay is inferred
from the charge of the lepton from semileptonic B decay. The
initial flavor is inferred by determining the flavor of the
other B hadron produced in the collision, either from its
semileptonic decay (soft-lepton tag) or from its jet charge.
The measurement yields (Formula presented), where the first
uncertainty is statistical and the second uncertainty is
systematic. The statistical powers (Formula presented) of
the soft-lepton and jet-charge flavor taggers are (Formula
presented) and (Formula presented), respectively. © 1999
The American Physical Society.},
Doi = {10.1103/PhysRevD.60.072003},
Key = {fds314164}
}
@article{fds314156,
Author = {al, FAE},
Title = {``Measurement of $Z^{0}$ and Drell-Yan Production Cross
Sections using Dimuons in $p\overline p$ Collisions at
$\sqrt{s} = 1.8$ TeV,"},
Journal = {Physical Review},
Volume = {D59},
Number = {5},
Pages = {052002},
Publisher = {American Physical Society (APS)},
Year = {1999},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.59.052002},
Abstract = {We present a measurement of [Formula Presented] boson and
Drell-Yan production cross sections in [Formula Presented]
collisions at [Formula Presented] using a sample of [Formula
Presented] accumulated by the Collider Detector at Fermilab.
The Drell-Yan cross section is measured in the mass range of
[Formula Presented] We compare the measurements with the
predictions of quantum chromodynamics in both leading order
and next-to-leading order, incorporating the recent parton
distribution functions. The measurements are consistent with
the standard model expectations. © 1999 The American
Physical Society.},
Doi = {10.1103/PhysRevD.59.052002},
Key = {fds314156}
}
@article{fds314161,
Author = {al, TAE},
Title = {``Measurement of the $B^0 \overline{B^0}$ Oscillation
Frequency using $lÐD^{*+}$ Pairs and Lepton Flavor
Tags,"},
Journal = {Physical Review},
Volume = {D60},
Number = {11},
Pages = {112004},
Publisher = {American Physical Society (APS)},
Year = {1999},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.60.112004},
Abstract = {The oscillation frequency (Formula presented) of (Formula
presented) mixing is measured using the partially
reconstructed semileptonic decay (Formula presented) The
data sample was collected with the CDF detector at the
Fermilab Tevatron collider during 1992–1995 by triggering
on the existence of two lepton candidates in an event, and
corresponds to about 110 (Formula presented) of (Formula
presented) collisions at (Formula presented) TeV. We
estimate the proper decay time of the (Formula presented)
meson from the measured decay length and reconstructed
momentum of the (Formula presented) system. The charge of
the lepton in the final state identifies the flavor of the
(Formula presented) meson at its decay. The second lepton in
the event is used to infer the flavor of the (Formula
presented) meson at production. We measure the oscillation
frequency to be (Formula presented) (Formula presented),
where the first uncertainty is statistical and the second is
systematic. © 1999 The American Physical
Society.},
Doi = {10.1103/PhysRevD.60.112004},
Key = {fds314161}
}
@article{fds314154,
Author = {al, FAE},
Title = {``Measurement of the $B^-$ and $\overline B^0$ Meson
Lifetimes using Semileptonic Decays,"},
Journal = {Physical Review},
Volume = {D58},
Number = {3},
Pages = {092002},
Publisher = {American Physical Society (APS)},
Year = {1998},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.59.032004},
Abstract = {The lifetime of the [Formula Presented] meson is measured
using the semileptonic decay [Formula Presented] The data
sample consists of about [Formula Presented] of [Formula
Presented] collisions at [Formula Presented] collected by
the CDF detector at Fermilab. Four different [Formula
Presented] decay modes are reconstructed resulting in
approximately 600 [Formula Presented] signal events. The
[Formula Presented] meson lifetime is determined to be
[Formula Presented] where the first and second uncertainties
are statistical and systematic, respectively. The [Formula
Presented] meson decay length distribution is examined for a
lifetime difference [Formula Presented] between the two mass
eigenstates of the [Formula Presented] meson. An upper limit
of ΔΓ/Γ<0.83 is set at the 95% confidence level. © 1999
The American Physical Society.},
Doi = {10.1103/PhysRevD.59.032004},
Key = {fds314154}
}
@article{fds314153,
Author = {al, FAE},
Title = {``Measurement of the $B_d^0\overline{B_{d}^0}$ Oscillation
Frequency using Dimuon Data in $p\overline p$ Collisions at
$\sqrt{s} = 1.8$ TeV,"},
Journal = {Physical Review},
Volume = {D60},
Number = {5},
Pages = {051101},
Publisher = {American Physical Society (APS)},
Year = {1999},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.60.051101},
Abstract = {We present a measurement of the mass difference (Formula
presented) of the two (Formula presented) mass eigenstates.
We use a flavor tagging method based on the lepton charge,
in a sample of events with two muons at low transverse
momentum. The sample corresponds to an integrated luminosity
of (Formula presented) collected by the Collider Detector at
Fermilab. The result obtained is (Formula presented) © 1999
The American Physical Society.},
Doi = {10.1103/PhysRevD.60.051101},
Key = {fds314153}
}
@article{fds321375,
Author = {al, FAE},
Title = {``Measurement of the $B_{d}^{0}$-$\overline {B_{d}^{0}}$
Flavor Oscillation Frequency and Study of Same Side Flavor
Tagging of $B$ Mesons in $p\overline p$ Collisions,"},
Journal = {Physical Review},
Volume = {D59},
Number = {3},
Pages = {032001},
Publisher = {American Physical Society (APS)},
Year = {1999},
url = {http://dx.doi.org/10.1103/PhysRevD.59.032001},
Abstract = {[Formula Presented] oscillations are observed in
“self-tagged” samples of partially reconstructed
[Formula Presented] mesons decaying into a lepton and a
charmed meson collected in [Formula Presented] collisions at
[Formula Presented] A flavor tagging technique is employed
which relies upon the correlation between the flavor of
[Formula Presented] mesons and the charge of a nearby
particle. We measure the flavor oscillation frequency to be
[Formula Presented] The tagging method is also demonstrated
in exclusive samples of [Formula Presented] and [Formula
Presented] where similar flavor-charge correlations are
observed. The tagging characteristics of the various samples
are compared with each other, and with Monte Carlo
simulations. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevD.59.032001},
Key = {fds321375}
}
@article{fds321376,
Author = {al, FAE},
Title = {``Measurement of the $B_{S}^{0}$ Meson Lifetime using
Semileptonic Decays,"},
Journal = {Physical Review},
Volume = {D59},
Number = {9},
Pages = {032004},
Publisher = {American Physical Society (APS)},
Year = {1999},
url = {http://dx.doi.org/10.1103/PhysRevD.58.092002},
Abstract = {The lifetimes of the [Formula Presented] and [Formula
Presented] mesons are measured using the partially
reconstructed semileptonic decays [Formula Presented] where
[Formula Presented] is either a [Formula Presented] or
[Formula Presented] meson. The data were collected by the
CDF detector at the Fermilab Tevatron collider during
1992–1995 and correspond to about [Formula Presented] of
[Formula Presented] collisions at [Formula Presented] We
measure decay lengths and extract the lifetimes to be
[Formula Presented] ps and [Formula Presented] and the ratio
of the lifetimes to be [Formula Presented] where the first
uncertainties are statistical and the second are systematic.
© 1998 The American Physical Society.},
Doi = {10.1103/PhysRevD.58.092002},
Key = {fds321376}
}
@article{fds308817,
Author = {al, FAE},
Title = {``Measurement of the Associated $\gamma + \mu^{\pm}$
Production Cross Section in $p\overline p$ Collisions at
$\sqrt{s} = 1.8$ TeV,"},
Journal = {Physical Review},
Volume = {D60},
Number = {9},
Pages = {092003},
Year = {1999},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.60.092003},
Abstract = {We present the first measurement of associated direct
photon(Formula presented)muon production in hadronic
collisions, from a sample of 1.8 TeV (Formula presented)
collisions recorded with the Collider Detector at Fermilab.
Quantum chromodynamics (QCD) predicts that these events are
primarily from the Compton scattering process (Formula
presented) with the final state charm quark producing a
muon. Hence this measurement is sensitive to the charm quark
content of the proton. The measured cross section of
(Formula presented) pb is compared to a leading-order QCD
parton shower model as well as a next-to-leading-order QCD
calculation. © 1999 The American Physical
Society.},
Doi = {10.1103/PhysRevD.60.092003},
Key = {fds308817}
}
@article{fds308833,
Author = {al, FAE},
Title = {``Measurement of the Differential Cross Section for Events
with Large Total Transverse Energy in $p\overline p$
Collisions at $\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review Letters},
Volume = {80},
Number = {16},
Pages = {3461},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.3461},
Abstract = {We present a measurement of the differential cross section
dσ/dΣEjetT for the production of multijet events in pp
collisions where the sum is over all jets with transverse
energy EjetT > EminT. The measured cross section for events
with EjetT > 320 GeV is compared to O(α3s) perturbative QCD
predictions and QCD parton shower Monte Carlo predictions.
The agreement between the O(α3s) predicted and observed
event rates is reasonable for EminT = 100 GeV, but poorer
for EminT = 20 GeV. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.80.3461},
Key = {fds308833}
}
@article{fds308773,
Author = {al, TAE},
Title = {``Measurement of the Top Quark $p_T$ Distribution,''},
Journal = {Physical Review Letters},
Volume = {87},
Number = {10},
Pages = {102001},
Year = {2001},
url = {http://dx.doi.org/10.1103/physrevlett.87.102001},
Abstract = {We have measured the p(T) distribution of top quarks that
are pair produced in pp collisions at sqrt[s] = 1.8 TeV
using a sample of tt decays in which we observe a single
high- p(T) charged lepton, a neutrino, and four or more
jets. We use a likelihood technique that corrects for the
experimental bias introduced due to event reconstruction and
detector resolution effects. The observed distribution is
consistent with the standard model prediction. We use these
data to place limits on the production of high- p(T) top
quarks suggested in some models of anomalous top quark pair
production.},
Doi = {10.1103/physrevlett.87.102001},
Key = {fds308773}
}
@article{fds326111,
Author = {al, TAE},
Title = {``Measurement of the two-jet differential cross section in
\ppb collisions at $\sqrt{s} = 1800$ GeV,''},
Journal = {Physical Review},
Volume = {D64},
Number = {1},
Pages = {012001},
Year = {2001},
url = {http://dx.doi.org/10.1103/PhysRevD.64.012001},
Abstract = {A measurement is presented of the two-jet differential cross
section [Formula Presented] at center of mass energy
[Formula Presented] GeV in [Formula Presented] collisions.
The results are based on an integrated luminosity of 86
[Formula Presented] collected during 1994 to 1995 by the CDF
Collaboration at the Fermilab Tevatron collider. The
differential cross section is measured as a function of the
transverse energy [Formula Presented] of a jet in the
pseudorapidity region [Formula Presented] for four different
pseudorapidity bins of a second jet restricted to [Formula
Presented] The results are compared with next-to-leading
order QCD calculations determined using the CTEQ4 and MRST
sets of parton distribution functions. None of the sets
examined in this analysis provides a good description of the
data. © 2001 The American Physical Society.},
Doi = {10.1103/PhysRevD.64.012001},
Key = {fds326111}
}
@article{fds357484,
Author = {al, FAE},
Title = {``Observation of $B^{+}\rightarrow\psi$(2S)$K^{+}$ and
$B^{0}\rightarrow\psi(2S)K^{*}(892)^{0}$ Decays and
Measurements of $B$-Meson Branching Fractions into $J/\psi$
and $\psi$(2S) Final States,"},
Journal = {Physical Review},
Volume = {D58},
Number = {7},
Pages = {112004},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevD.58.072001},
Doi = {10.1103/PhysRevD.58.072001},
Key = {fds357484}
}
@article{fds314160,
Author = {al, FAE},
Title = {``Observation of $B_{c}$ Mesons in $p\overline p$ Collisions
at $\sqrt{s} = 1.8$ TeV,"},
Journal = {Physical Review},
Volume = {D58},
Number = {11},
Pages = {112004},
Publisher = {American Physical Society (APS)},
Year = {1998},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.58.112004},
Abstract = {We report the observation of bottom-charmed mesons [Formula
Presented] in 1.8 TeV [Formula Presented] collisions using
the CDF detector at the Fermilab Tevatron. The [Formula
Presented] mesons were found through their semileptonic
decays, [Formula Presented] A fit to the [Formula Presented]
mass distribution yielded [Formula Presented] events from
[Formula Presented] mesons. A test of the null hypothesis,
i.e., an attempt to fit the data with background alone, was
rejected at the level of 4.8 standard deviations. By
studying the quality of the fit as a function of the assumed
[Formula Presented] mass, we determined [Formula Presented]
From the distribution of trilepton intersection points in
the plane transverse to the beam direction we measured the
[Formula Presented] lifetime to be [Formula Presented] We
also measured the ratio of production cross section times
branching fraction for [Formula Presented] relative to that
for [Formula Presented] to be [Formula Presented] © 1998
The American Physical Society.},
Doi = {10.1103/PhysRevD.58.112004},
Key = {fds314160}
}
@article{fds331485,
Author = {al, TAE},
Title = {``Observation of Diffractive $b$-Quark Production at the
Fermilab Tevatron,"},
Journal = {Physical Review Letters},
Volume = {84},
Number = {2},
Pages = {232},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevLett.84.232},
Abstract = {We report a measurement of the fraction of b quarks produced
diffractively in ⊯pp collisions at √ s = 1.8 TeV.
Diffraction is identified by the absence of particles in a
forward pseudorapidity region. From events with an electron
of transverse momentum 9.5 < peT< 20 GeV/c within the
pseudorapidity region |η| < 1.1, the ratio of diffractive
to total b-quark production rates is found to be R⊯bb=
[0.62 ± 0.19(stat) ± 0.16(syst)]%. This result is
comparable in magnitude to corresponding ratios for W and
dijet production but significantly lower than expectations
based on factorization. © 2000 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.84.232},
Key = {fds331485}
}
@article{fds331639,
Author = {al, TAE},
Title = {``Observation of orbitally excited $B$ mesons in \ppb
collisions at $\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review},
Volume = {D64},
Number = {7},
Pages = {072002},
Year = {2001},
url = {http://dx.doi.org/10.1103/PhysRevD.64.072002},
Abstract = {We measure the relative rate of production of orbitally
excited [Formula Presented] states of B mesons [Formula
Presented] by observing their decays into [Formula
Presented] We reconstruct B mesons through semileptonic
decay channels using data collected in [Formula Presented]
collisions at [Formula Presented] The fraction of light B
mesons that are produced as [Formula Presented] states is
measured to be [Formula Presented] We also measure the
collective mass of the [Formula Presented] states, and
quantify the result by quoting the (model-dependent) mass of
the lowest [Formula Presented] state to be [Formula
Presented] © 2001 The American Physical
Society.},
Doi = {10.1103/PhysRevD.64.072002},
Key = {fds331639}
}
@article{fds308847,
Author = {al, FAE},
Title = {``Properties of Photon Plus Two-Jet Events in $\overline pp$
Collisions at $\sqrt s$ =1.8 TeV,''},
Journal = {Physical Review},
Volume = {D57},
Number = {1},
Pages = {67},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevD.57.67},
Abstract = {We present the first general measurements (invariant-mass,
transverse-energy, and angular distributions) of the
process, (Formula presented) (Formula presented) using data
collected by the CDF at Fermilab. We compare the data with
predictions from a tree-level QCD calculation and the PYTHIA
shower Monte Carlo program. Our data sample is particularly
sensitive to contributions from initial- and final-state
radiation of photons and jets. Using the PYTHIA Monte Carlo
program, we contrast the kinematical distributions for
direct photon production with those for initial- and
final-state photon radiation (bremsstrahlung). Based on the
angular distributions, we find that our data favor a mixture
of bremsstrahlung and direct photon production, as
predicted, over either process alone. © 1998 The American
Physical Society.},
Doi = {10.1103/PhysRevD.57.67},
Key = {fds308847}
}
@article{fds308793,
Author = {al, TAE},
Title = {``Search for Color Singlet Technicolor Particles in
$p\overline p$ Collisions at $\sqrt{s} = 1.8$
TeV,"},
Journal = {Physical Review Letters},
Volume = {84},
Number = {6},
Pages = {1110},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevLett.84.1110},
Abstract = {We search for color singlet technirho and technipion
production in pp¯ Collisions at √s = 1.8TeVrecorded with
the Collider Detector at Fermilab. These exotic technimesons
are present in a model of walking technicolor. The
signatures studied are lepton plus two jets plus ET and
multijet final states. No excess of events is seen in either
final state. We set an upper limit on the technirho
production cross section and exclude a region in the
technipion mass versus technirho mass plane. © 2000
American Physical Society.},
Doi = {10.1103/PhysRevLett.84.1110},
Key = {fds308793}
}
@article{fds308846,
Author = {al, FAE},
Title = {``Search for Flavor-Changing Neutral Current Decays of the
Top Quark in $p\overline p$ Collisions at $\sqrt{s} = 1.8$
TeV,''},
Journal = {Physical Review Letters},
Volume = {80},
Number = {12},
Pages = {2525},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.2525},
Abstract = {We search for the flavor-changing neutral current decays of
the top quark t → λ and t → qZ (here represents the c
and u quarks) in pp collisions at √s = 1.8 TeV. We use a
dataset (∫ L dt˜ 110pb-1) collected during the 1992-1995
run of the Collider Detector at Fermilab. We set 95%
confidence level limits on the branching fractions B(t →
qλ) < 3.2% and B(t → qZ) < 33%, consistent with the
standard model. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.80.2525},
Key = {fds308846}
}
@article{fds330937,
Author = {al, TAE},
Title = {``Search for Gluinos and Squarks Using Like-Sign Dileptons
in \ppb Collisions at $\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review Letters},
Volume = {87},
Number = {25},
Pages = {251803},
Year = {2001},
url = {http://dx.doi.org/10.1103/physrevlett.87.251803},
Abstract = {We present results of the first search for like-sign
dilepton ( e(+/-)e(+/-), e(+/-)mu(+/-), mu(+/-)mu(+/-))
events associated with multijets and large missing energy
using 106 pb(-1) of data in pp macro collisions at square
root of s = 1.8 TeV collected during 1992-1995 by the CDF
experiment. Finding no events that pass our selection, we
examine pair production of gluinos (tilde g) and squarks
(tilde q) in a constrained framework of the minimal
supersymmetric standard model. At tan beta = 2 and mu = -800
GeV/c(2), we set 95% confidence level limits of M(tilde
g)>221 GeV/c(2) for M(tilde g) approximately M(tilde q), and
M(tilde q)>168 GeV/c(2) for M(tilde q)>>M(tilde g), both
with small variation as a function of mu.},
Doi = {10.1103/physrevlett.87.251803},
Key = {fds330937}
}
@article{fds321378,
Author = {al, FAE},
Title = {``Search for Long-Lived Parents of $Z^{0}$ Bosons in
$p\overline p$ Collisions at $\sqrt{s} = 1.8$
TeV,"},
Journal = {Physical Review},
Volume = {D58},
Number = {5},
Pages = {051102},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevD.58.051102},
Abstract = {We search for new long-lived particles which decay to
[Formula Presented] bosons by looking for [Formula
Presented] decays with displaced vertices. We find no
evidence for parent particles of the [Formula Presented]
with long lifetimes in [Formula Presented] of data from the
CDF experiment at Fermilab. We set a cross section limit as
a function of the lifetime of the parent particle for both a
generic [Formula Presented] parent and a fourth-generation,
charge [Formula Presented] quark that decays into [Formula
Presented]. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevD.58.051102},
Key = {fds321378}
}
@article{fds308774,
Author = {al, TAE},
Title = {``Search for Neutral Supersymmetric Higgs Bosons in \ppb
Collisions at $\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review Letters},
Volume = {86},
Number = {20},
Pages = {4472},
Year = {2001},
url = {http://dx.doi.org/10.1103/physrevlett.86.4472},
Abstract = {We present the results of a search for neutral Higgs bosons
produced in association with b quarks in pp-->bb(phi)-->bbb
final states with 91+/-7 pb(-1) of pp collisions at sqrt[s]
= 1.8 TeV recorded by the Collider Detector at Fermilab. We
find no evidence of such a signal and the data are
interpreted in the context of the neutral Higgs sector of
the minimal supersymmetric extension of the standard model.
With basic parameter choices for the supersymmetric scale
and the stop-quark mixing, we derive 95% C.L. lower mass
limits for neutral Higgs bosons for tan(beta) values in
excess of 35.},
Doi = {10.1103/physrevlett.86.4472},
Key = {fds308774}
}
@article{fds323773,
Author = {al, FAE},
Title = {``Search for New Physics in Diphoton Events in $p\overline
p$ Collisions at $\sqrt{s} = 1.8$ TeV,"},
Journal = {Physical Review},
Volume = {D59},
Number = {9},
Pages = {092002},
Publisher = {American Physical Society (APS)},
Year = {1999},
url = {http://dx.doi.org/10.1103/PhysRevD.59.092002},
Abstract = {We present a detailed description of a search for anomalous
production of missing [Formula Presented] [Formula
Presented] jets, leptons [Formula Presented] b quarks, or
additional photons in events containing two isolated,
central [Formula Presented] photons with [Formula Presented]
The results are consistent with standard model expectations,
with the possible exception of one event that has, in
addition to the two photons, a central electron, a
high-[Formula Presented] electromagnetic cluster, and large
[Formula Presented] We set limits using two specific SUSY
scenarios for production of diphoton events with [Formula
Presented] © 1999 The American Physical
Society.},
Doi = {10.1103/PhysRevD.59.092002},
Key = {fds323773}
}
@article{fds330941,
Author = {al, FAE},
Title = {``Search for R-parity Violating Supersymmetry using
Like-Sign Dielectrons in $p\overline p$ Collisions at
$\sqrt{s} = 1.8$ TeV,"},
Journal = {Physical Review Letters},
Volume = {83},
Number = {11},
Pages = {2133},
Publisher = {American Physical Society (APS)},
Year = {1999},
url = {http://dx.doi.org/10.1103/PhysRevLett.83.2133},
Abstract = {We present a search for like-sign dielectron plus multijet
events using 107pb of data in pp collisons at √ s = 1.8
TeV collected in 1992-1995 by the CDF experiment. Finding no
events that pass our selection we set σ × BR limits on two
supersymmetric processes that can produce this experimental
signature: gluino-gluino or squark-antisquark production
with R-parity violating decays of the charm squark or
lightest neutralino via a nonzero λ′ coupling. We compare
our results to the next-to-leading order calculations for
gluino and squark production cross sections and set lower
limits on M( g) M( t ) and M( q). © 1999 The American
Physical Society. − 1 ∼ ∼ ∼ 121 1},
Doi = {10.1103/PhysRevLett.83.2133},
Key = {fds330941}
}
@article{fds331642,
Author = {al, TAE},
Title = {``Search for scalar top quark production in $p\overline p$
Collisions at $\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review Letters},
Volume = {84},
Number = {23},
Pages = {5273},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevLett.84.5273},
Abstract = {We have searched for direct production of scalar top quarks
at the Collider Detector at Fermilab in 88pb-1of p⊯p
collisions at vs=1.8TeV. We assume the scalar top quark
decays into either a bottom quark and a chargino or a bottom
quark, a lepton, and a scalar neutrino. The event signature
for both decay scenarios is a lepton, missing transverse
energy, and at least two b-quark jets. For a chargino mass
of 90GeV/c2and scalar neutrino masses of at least 40GeV/c2,
we find no evidence for scalar top production and present
upper limits on the production cross section in both decay
scenarios. © 2000 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.84.5273},
Key = {fds331642}
}
@article{fds308798,
Author = {al, TAE},
Title = {``Search for second and third generation leptoquarks
including production via technicolor interactions in
$p\overline p$ Collisions at $\sqrt{s} = 1.8$
TeV,''},
Journal = {Physical Review Letters},
Volume = {85},
Number = {10},
Pages = {2056},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevLett.85.2056},
Abstract = {The collider detector at Fermilab was used to examine second
and third generation leptoquarks. The potential production
of color triplet technipions in strongly-coupled color octet
technirhos decays was examined. Events with heavy flavor
jets and missing energy may indicate the second-generation
leptoquark decay to a charm quark and neutrino. Since there
were no excess of events above standard model predictions,
95% confidence level limits were determined.},
Doi = {10.1103/PhysRevLett.85.2056},
Key = {fds308798}
}
@article{fds308835,
Author = {al, FAE},
Title = {``Search for Second Generation Leptoquarks in the Dimuon
plus Dijet Channel of $p\overline p$ Collisions at $\sqrt{s}
= 1.8$ TeV,"},
Journal = {Physical Review Letters},
Volume = {81},
Number = {22},
Pages = {4806},
Publisher = {American Physical Society (APS)},
Year = {1998},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.4806},
Abstract = {We report on a search for second generation leptoquarks(Φ2)
using a data sample corresponding to an integrated
luminosity of 110 pb−1 collected at the Collider Detector
at Fermilab. We present upper limits on the production cross
section as a function of Φ2 mass, assuming that the
leptoquarks are produced in pairs and decay into a muon and
a quark with branching ratio MΦ2 > 202(160)GeV/c2 at 95%
confidence level for scalar leptoquarks with β = 1(0.5). ©
1998 American Physical Society.},
Doi = {10.1103/PhysRevLett.81.4806},
Key = {fds308835}
}
@article{fds323771,
Author = {al, TAE},
Title = {``Search for the charged Higgs boson in the decays of top
quark pairs in the $e \tau$ and $\mu \tau$ channels at
$\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review},
Volume = {D62},
Number = {1},
Pages = {012004},
Publisher = {American Physical Society (APS)},
Year = {2000},
url = {http://dx.doi.org/10.1103/PhysRevD.62.012004},
Abstract = {Top quark production offers the unique opportunity to search
for a charged Higgs boson (Formula presented) as the
contribution from (Formula presented) can be large in
extensions of the standard model. We use results from a
search for top quark pair production by the Collider
Detector at Fermilab (CDF) in the (Formula presented) and
(Formula presented) signatures to set an upper limit on the
branching ratio of (Formula presented) in 106 (Formula
presented) of data. The upper limit is in the range 0.5 to
0.6 at 95% C.L. for (Formula presented) masses in the range
60 to 160 GeV, assuming the branching ratio for (Formula
presented) is 100%. The (Formula presented) lepton is
detected through its 1-prong and 3-prong hadronic decays. ©
2000 The American Physical Society.},
Doi = {10.1103/PhysRevD.62.012004},
Key = {fds323771}
}
@article{fds308510,
Author = {al, TAE},
Title = {``Search for the supersymmetric partner of the top quark in
\pbp collisions at $\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review},
Volume = {D63},
Number = {9},
Pages = {091101},
Year = {2001},
url = {http://dx.doi.org/10.1103/PhysRevD.63.091101},
Abstract = {We report on a search for the supersymmetric partner of the
top quark (top squark) produced in [Formula Presented]
events using [Formula Presented] of [Formula Presented]
collisions at [Formula Presented] recorded with the Collider
Detector at Fermilab. In the case of a light top squark, the
decay of the top quark into a top squark plus the lightest
supersymmetric particle (LSP) could have a significant
branching ratio. The observed events are consistent with
standard model [Formula Presented] production and decay.
Hence, we set limits on the branching ratio of the top quark
decaying into a top squark plus LSP, excluding branching
ratios above 45% for a LSP mass up to [Formula Presented] ©
2001 The American Physical Society.},
Doi = {10.1103/PhysRevD.63.091101},
Key = {fds308510}
}
@article{fds308811,
Author = {al, FAE},
Title = {``Search for Third-Generation Leptoquarks from Technicolor
Models in $p\overline p$ Collisions at $\sqrt{s} = 1.8$
TeV,"},
Journal = {Physical Review Letters},
Volume = {82},
Number = {16},
Pages = {3206},
Publisher = {American Physical Society (APS)},
Year = {1999},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.3206},
Abstract = {We report the results of a search for technicolor using
110pb-1 of pp collisions recorded by the Collider Detector
at Fermilab (CDF). In technicolor models containing a
technifamily, color-octet technirhos enhance the pair
production of color-triplet technipions, which behave as
third-generation leptoquarks. From our previously reported
search for third-generation leptoquarks, we present
constraints on the production of color-triplet technipions
and color-octet technirhos as a function of their masses. ©
1999 The American Physical Society.},
Doi = {10.1103/PhysRevLett.82.3206},
Key = {fds308811}
}
@article{fds323770,
Author = {al, TAE},
Title = {``Tests of enhanced leading order QCD in $W$ boson plus jets
events from 1.8 TeV \pbp collisions,''},
Journal = {Physical Review},
Volume = {D63},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society (APS)},
Year = {2001},
url = {http://dx.doi.org/10.1103/PhysRevD.63.072003},
Abstract = {We present a study of events with W bosons and hadronic jets
produced in [Formula Presented] collisions at a center of
mass energy of 1.8 TeV. The data consist of 51400 [Formula
Presented] decay candidates from 108 [Formula Presented] of
integrated luminosity collected using the CDF detector at
the Fermilab Tevatron collider. Cross sections and jet
production properties have been measured for [Formula
Presented] to [Formula Presented] jet events. The data
compare well to predictions of leading-order QCD matrix
element calculations with added gluon radiation and
simulated parton fragmentation. © 2001 The American
Physical Society.},
Doi = {10.1103/PhysRevD.63.072003},
Key = {fds323770}
}
@article{fds308591,
Author = {Aaltonen, and T, and others},
Title = {{Cross Section Constrained Top Quark Mass Measurement from
Dilepton Events at the Tevatron}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {6},
Pages = {062005},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.062005},
Abstract = {We report the first top-quark mass measurement that uses a
cross-section constraint to improve the mass determination.
This measurement is made with a dilepton $t\bar{t}$ event
candidate sample collected with the Collider Detector II at
Fermilab. From a data sample corresponding to an integrated
luminosity of 1.2 fb-1, we measure a top-quark mass of
170.7-3.9+4.2(stat)\pm 2.6(syst)\pm 2.4(theory) GeV/c2. The
measurement without the cross-section constraint is
169.7-4.9+5.2(stat)\pm 3.1(syst) GeV/c2.},
Doi = {10.1103/physrevlett.100.062005},
Key = {fds308591}
}
@article{fds308615,
Author = {Aaltonen, and T, and others},
Title = {{Cross section measurements of high-pT dilepton final-state
processes using a global fitting method}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {1},
Pages = {012003},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://arxiv.org/pdf/hep-ex/0612058},
Abstract = {We present a new method for studying high-pT dilepton events
$(e^\pm e^{-/+}, \mu^\pm \mu^{-/+}, e^\pm\mu^{-/+})$ and
simultaneously extracting the production cross sections of
$p\bar{p}$-->$t\bar{t}$, $p\bar{p}$-->W+W-, and
$p\bar{p}$-->Z0-->tau+tau- at a center-of-mass energy of
$\sqrt{s}=1.96$ TeV. We perform a likelihood fit to the
dilepton data in a parameter space defined by the missing
transverse energy and the number of jets in the event. Our
results, which use 360 pb-1 of data recorded with the CDF II
detector at the Fermilab Tevatron Collider, are
sigma($t\bar{t}$)=8.5-2.2+2.7 pb, sigma(W+W-)=16.3-4.4+5.2
pb, and sigma(Z0-->tau+tau-)=291-46+50 pb.},
Doi = {10.1103/PhysRevD.78.012003},
Key = {fds308615}
}
@article{fds308586,
Author = {Aaltonen, and T, and others},
Title = {{Evidence for D0-D0bar mixing using the CDF II
Detector}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {12},
Pages = {121802},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.121802},
Abstract = {We measure the time dependence of the ratio of decay rates
for the rare decay D0-->K+pi- to the Cabibbo-favored decay
D0-->K-pi+. A signal of 12.7×103 D0-->K+pi- decays was
obtained using the Collider Detector at Fermilab II detector
at the Fermilab Tevatron with an integrated luminosity of
1.5 fb-1. We measure the D0-[overline D]0 mixing parameters
(RD,y[prime],x[prime]2), and find that the data are
inconsistent with the no-mixing hypothesis with a
probability equivalent to 3.8 Gaussian standard
deviations.},
Doi = {10.1103/physrevlett.100.121802},
Key = {fds308586}
}
@article{fds308583,
Author = {Aaltonen, and T, and others},
Title = {{First Flavor-Tagged Determination of Bounds on Mixing-
Induced CP Violation in Bs -> J/psi phi Decays}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {16},
Pages = {161802},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.161802},
Abstract = {This Letter describes the first determination of bounds on
the CP-violation parameter 2betas using Bs0 decays in which
the flavor of the bottom meson at production is identified.
The result is based on approximately 2000 Bs0-->J/psiphi
decays reconstructed in a 1.35 fb-1 data sample collected
with the CDF II detector using $p\bar{p}$ collisions
produced at the Fermilab Tevatron. We report confidence
regions in the two-dimensional space of 2betas and the
decay-width difference DeltaGamma. Assuming the standard
model predictions of 2betas and DeltaGamma, the probability
of a deviation as large as the level of the observed data is
15%, corresponding to 1.5 Gaussian standard
deviations.},
Doi = {10.1103/physrevlett.100.161802},
Key = {fds308583}
}
@article{fds308593,
Author = {Aaltonen, and T, and others},
Title = {{First observation of the decay $B^0_s \to D^-_s D^+_s$ and
measurement of its branching ratio}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {2},
Pages = {021803},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.021803},
Abstract = {We report the observation of the exclusive decay
Bs0-->Ds-Ds+ at the 7.5 standard deviation level using 355
pb-1 of data collected by the CDF II detector in $p\bar{p}$
collisions at $\sqrt{s}=1.96$ TeV at the Fermilab Tevatron.
We measure the relative branching ratio [script
B](Bs0-->Ds-Ds+)/[script B](B0-->D-Ds+) =1.44-0.44+0.48.
Using the world average value for [script B](B0-->D-Ds+), we
find [script B](Bs0-->Ds-Ds+) =(9.4-4.2+4.4)×10-3. This
provides a lower bound DeltaGammasCP/Gammas> =2[script
B](Bs0-->Ds-Ds+)>1.2×10-2 at 95% C.L.},
Doi = {10.1103/physrevlett.100.021803},
Key = {fds308593}
}
@article{fds308576,
Author = {Aaltonen, and T, and others},
Title = {{Forward-Backward Asymmetry in Top Quark Production in
$p\bar{p}$ Collisions at $sqrt{s}=1.96$ TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {101},
Number = {20},
Pages = {202001},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.202001},
Abstract = {We present measurements of the forward-backward charge
asymmetry in top pair production using 1.9 fb-1 of
$p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV recorded with
the Collider Detector at Fermilab II. Correcting for
acceptance and measurement dilutions we obtain parton-level
asymmetries of AFB$p\bar{p}$=0.17\pm 0.08 in the $p\bar{p}$
frame and AFB$t\bar{t}$=0.24+/-0.14 in the $t\bar{t}$ frame.
The values are consistent with the standard model
expectation and disfavor exotic production mechanisms with
significant negative values.},
Doi = {10.1103/physrevlett.101.202001},
Key = {fds308576}
}
@article{fds308607,
Author = {Aaltonen, and T, and others},
Title = {{Limits on the Production of Narrow $t\bar{t}$ Resonances in
$p\bar{p}$ Collisions at $\sqrt{s}=1.96$
TeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {5},
Pages = {051102},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.051102},
Abstract = {We search for evidence of resonant top quark pair production
in 955 pb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
recorded with the CDF II detector at the Fermilab Tevatron.
For fully reconstructed candidate $t\bar{t}$ events
triggered on leptons with large transverse momentum and
containing at least one identified b-quark jet, we compare
the invariant mass spectrum of $t\bar{t}$ pairs to the
expected superposition of standard model $t\bar{t}$,
non-$t\bar{t}$ backgrounds, and a simple resonance model
based on a sequential Z[prime] boson. We establish upper
limits for sigma($p\bar{p}$-->Z[prime])·Br(Z[prime]-->$t\bar{t}$)
in the Z[prime] mass interval from 450 GeV/c2 to 900 GeV/c2.
A topcolor leptophobic Z[prime] is ruled out below 720
GeV/c2, and the cross section of any narrow Z[prime]-like
state decaying to $t\bar{t}$ is found to be less than 0.64
pb at 95% C.L. for MZ[prime] above 700 GeV/c2.},
Doi = {10.1103/PhysRevD.77.051102},
Key = {fds308607}
}
@article{fds308612,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of $b$-jet Shapes in Inclusive Jet Production
in $p \bar{p}$ Collisions at $\sqrt{s}$ =
1.96-TeV}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {7},
Pages = {072005},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.072005},
Abstract = {We present a measurement of the shapes of b-jets using 300
pb-1 of data obtained with the upgraded Collider Detector at
Fermilab (CDF II) in $p \bar{p}$ collisions at
center-of-mass energy $\sqrt{s}=1.96$ TeV. This measurement
covers a wide transverse momentum range, from 52 to 300
GeV/c. Samples of heavy-flavor enhanced jets together with
inclusive jets are used to extract the average shapes of
b-jets. The b-jets are expected to be broader than inclusive
jets. Moreover, b-jets containing a single b-quark are
expected to be narrower than those containing a $b \bar{b}$
pair from gluon splitting. The measured b-jet shapes are
found to be significantly broader than expected from the
pythia and herwig Monte Carlo simulations. This effect may
arise from an underestimation of the fraction of b-jets
originating from gluon splitting in these simulations. The
jet shape distributions provided in this paper could be
compared to any full Monte Carlo simulation and could be
used to further constrain the various parameters.},
Doi = {10.1103/PhysRevD.78.072005},
Key = {fds308612}
}
@article{fds308595,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of correlated b-bbar production in ${p
\bar{p}}$ collisions at s**(1/2) = 1960 GeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {7},
Pages = {072004},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.072004},
Abstract = {We present a measurement of the correlated b[overline b]
production cross section. The data used in this analysis
were taken with the upgraded CDF detector (CDF II) at the
Fermilab Tevatron collider, and correspond to an integrated
luminosity of 742 pb-1. We utilize muon pairs with invariant
mass 5=3 GeV/c and |eta|=2 GeV/c and |y| mu,[overline b] -->
mu=1549\pm 133 pb. We compare this result with theoretical
predictions and previous measurements. We also report the
measurement of sigmac --> mu,[overline c] --> mu, a
by-product of the study of the background to b[overline b]
production.},
Doi = {10.1103/PhysRevD.77.072004},
Key = {fds308595}
}
@article{fds308587,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of Inclusive Jet Cross Sections in $Z/\gamma^*
(\to ee)+$ jets Production in $p\bar{p}$ Collisions at
$\sqrt{s}=1.96$ TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {10},
Pages = {102001},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.102001},
Abstract = {Inclusive jet cross sections in Z/gamma* events, with
Z/gamma* decaying into an electron-positron pair, are
measured as a function of jet transverse momentum and jet
multiplicity in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
with the upgraded Collider Detector at Fermilab in run II,
based on an integrated luminosity of 1.7 fb-1. The
measurements cover the rapidity region |yjet|Tjet>30 GeV/c.
Next-to-leading order perturbative QCD predictions are in
good agreement with the measured cross sections.},
Doi = {10.1103/physrevlett.100.102001},
Key = {fds308587}
}
@article{fds308585,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of Lifetime and Decay-Width Difference in
$B^0_s \to J/\psi \phi$ Decays}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {12},
Pages = {121803},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.121803},
Abstract = {We measure the mean lifetime ${\tau=2/(\Gamma_L+\Gamma_H)}$
and the decay-width difference ${\Delta\Gamma=\Gamma_L-\Gamma_H}$
of the light and heavy mass eigenstates of the ${B_s^0}$
meson, ${B_{sL}^0}$ and ${B_{sH}^0}$, in ${B_s^0\to
J/\psi\phi}$ decays using 1.7 fb-1 of data collected with
the CDF II detector at the Fermilab Tevatron $p\bar{p}$
collider. Assuming CP conservation, a good approximation for
the ${B_s^0}$ system in the standard model, we obtain
${\Delta\Gamma=0.076_{-0.063}^{+0.059}}$(stat)$\pm
0.006$(syst) ps-1 and $\tau=1.52\pm 0.04$(stat)$\pm
0.02$(syst) ps, the most precise measurements to date. Our
constraints on the weak phase and ${\Delta\Gamma}$ are
consistent with CP conservation.},
Doi = {10.1103/physrevlett.100.121803},
Key = {fds308585}
}
@article{fds308601,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of Ratios of Fragmentation Fractions for Bottom
Hadrons in $p \bar{p}$ Collisions at $\sqrt{s}$ =
1.96-TeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.072003},
Abstract = {This paper describes the first measurement of b-quark
fragmentation fractions into bottom hadrons in Run II of the
Tevatron Collider at Fermilab. The result is based on a 360
pb-1 sample of data collected with the CDF II detector in
$p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV. Semileptonic
decays of [overline B]0, B-, and [overline B]s0 mesons, as
well as Lambdab0 baryons, are reconstructed. For an
effective bottom hadron pT threshold of 7 GeV/c, the
fragmentation fractions are measured to be fu/fd=1.054\pm
0.018(stat)-0.045+0.025(sys)\pm 0.058([script B]),
fs/(fu+fd)=0.160\pm 0.005(stat)-0.010+0.011(sys)-0.034+0.057([script
B]), and fLambdab/(fu+fd)=0.281\pm 0.012(stat)-0.056+0.058(sys)-0.087+0.128([script
B]), where the uncertainty [script B] is due to
uncertainties on measured branching ratios. The value of
fs/(fu+fd) agrees within one standard deviation with
previous CDF measurements and the world average of this
quantity, which is dominated by LEP measurements. However,
the ratio fLambdab/(fu+fd) is approximately twice the value
previously measured at LEP. The approximately 2sigma
discrepancy is examined in terms of kinematic differences
between the two production environments.},
Doi = {10.1103/PhysRevD.77.072003},
Key = {fds308601}
}
@article{fds308610,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of the cross section for ${W}$-boson production
in association with jets in $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {6},
Pages = {011108},
Publisher = {American Physical Society (APS)},
Year = {2008},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1007/JHEP06(2013)084},
Abstract = {We present a measurement of the cross section for W-boson
production in association with jets in $p\bar{p}$ collisions
at $\sqrt{s}=1.96$ TeV. The analysis uses a data sample
corresponding to an integrated luminosity of 320 pb-1
collected with the CDF II detector. W bosons are identified
in their electron decay channel and jets are reconstructed
using a cone algorithm. For each W+>=n-jet sample (n=1-4) we
measure the differential cross section dsigma($p\bar{p}$-->W+>=n-jet)/dETnth-jet×[script
B](W-->enu) with respect to the transverse energy ET of the
nth-highest ET jet above 20 GeV, and the total cross section
sigma($p\bar{p}$-->W+>=n-jet;ETnth-jet>25 GeV)×[script
B](W-->enu), for a restricted W-->enu decay phase space. The
cross sections, corrected for all detector effects, can be
directly compared to particle level W+jet(s) predictions. We
present here comparisons to leading order and
next-to-leading order predictions.},
Doi = {10.1007/JHEP06(2013)084},
Key = {fds308610}
}
@article{fds308613,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of the Inclusive Jet Cross Section at the
Fermilab Tevatron $p \bar{p}$ Collider Using a Cone-Based
Jet Algorithm}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {5},
Pages = {052006},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.052006},
Abstract = {We present a measurement of the inclusive jet cross section
in $p \bar{p}$ collisions at $\sqrt{s}=1.96$ TeV based on
data collected by the CDF II detector with an integrated
luminosity of 1.13 fb-1. The measurement was made using the
cone-based midpoint jet clustering algorithm in the rapidity
region of |y|},
Doi = {10.1103/PhysRevD.78.052006},
Key = {fds308613}
}
@article{fds308598,
Author = {Aaltonen, and T, and others},
Title = {{Model-Independent and Quasi-Model-Independent Search for
New Physics at CDF}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {1},
Pages = {012002},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.012002},
Abstract = {Data collected in run II of the Fermilab Tevatron are
searched for indications of new electroweak scale physics.
Rather than focusing on particular new physics scenarios,
CDF data are analyzed for discrepancies with respect to the
standard model prediction. A model-independent approach
(Vista) considers the gross features of the data and is
sensitive to new large cross section physics. A
quasi-model-independent approach (Sleuth) searches for a
significant excess of events with large summed transverse
momentum and is particularly sensitive to new electroweak
scale physics that appears predominantly in one final state.
This global search for new physics in over 300 exclusive
final states in 927 pb-1 of $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV reveals no such significant indication
of physics beyond the standard model.},
Doi = {10.1103/PhysRevD.78.012002},
Key = {fds308598}
}
@article{fds308603,
Author = {Aaltonen, and T, and others},
Title = {{Observation of Exclusive Dijet Production at the Fermilab
Tevatron ${p \bar{p}}$ Collider}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {5},
Pages = {052004},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.052004},
Abstract = {We present the first observation and cross section
measurement of exclusive dijet production in [overline p]p
interactions, [overline p]p-->[overline p]+dijet+p. Using a
data sample of 310 pb-1 collected by the Run II Collider
Detector at Fermilab at $\sqrt{s}=1.96$ TeV, exclusive cross
sections for events with two jets of transverse energy
ETjet>=10 GeV have been measured as a function of minimum
ETjet. The exclusive signal is extracted from fits to data
distributions based on Monte Carlo simulations of expected
dijet signal and background shapes. The simulated background
distribution shapes are checked in a study of a largely
independent data sample of 200 pb-1 of b-tagged jet events,
where exclusive dijet production is expected to be
suppressed by the Jz=0 total angular momentum selection
rule. Results obtained are compared with theoretical
expectations, and implications for exclusive Higgs boson
production at the pp Large Hadron Collider at sqrt(s)=14 TeV
are discussed.},
Doi = {10.1103/PhysRevD.77.052004},
Key = {fds308603}
}
@article{fds308589,
Author = {Aaltonen, and T, and others},
Title = {{Observation of Orbitally Excited ${B_s}$
Mesons}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {8},
Pages = {082001},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.082001},
Abstract = {We report the observation of two narrow resonances
consistent with states of orbitally excited (L=1) Bs mesons
using 1 fb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
collected with the Collider Detector at Fermilab II detector
at the Fermilab Tevatron. We use two-body decays into K- and
B+ mesons reconstructed as B+-->J/psiK+, J/psi-->\mu^+\mu^-
or B+-->[overline D]0pi+, [overline D]0-->K+pi-. We deduce
the masses of the two states to be m(Bs1)=5829.4\pm 0.7
MeV/c2 and m(Bs2*)=5839.6\pm 0.7 MeV/c2.},
Doi = {10.1103/physrevlett.100.082001},
Key = {fds308589}
}
@article{fds308600,
Author = {Aaltonen, and T, and others},
Title = {{Search for chargino-neutralino production in ${p \bar{p}}$
collisions at 1.96 TeV with high pT leptons}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {5},
Pages = {052002},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.052002},
Abstract = {We present a search for the associated production of
charginos and neutralinos in $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV. The data were collected at the Collider
Detector at Fermilab (CDF II) and correspond to integrated
luminosities between 0.7 and 1.0 fb-1. We look for final
states with one high-pT electron or muon, and two additional
leptons. Our results are consistent with the standard model
expectations, and we set limits on the cross section as a
function of the chargino mass in three different
supersymmetric scenarios. For a specific minimal
supersymmetric standard model scenario with no slepton
mixing, we set a 95% C.L. limit at 151 GeV/c2.},
Doi = {10.1103/PhysRevD.77.052002},
Key = {fds308600}
}
@article{fds308579,
Author = {Aaltonen, and T, and others},
Title = {{Search for Doubly Charged Higgs Bosons with Lepton-Flavor-
Violating Decays involving Tau Leptons}},
Journal = {Phys. Rev. Lett.},
Volume = {101},
Number = {12},
Pages = {121801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.121801},
Abstract = {We search for pair production of doubly charged Higgs
particles ($H^{\pm\pm}$) followed by decays into
electron-tau (etau) and muon-tau (mu tau) pairs using data
(350 pb-1) collected from $\bar{p} p$ collisions at
$\sqrt{s}=1.96$ TeV by the CDF II experiment. We search
separately for cases where three or four final-state leptons
are detected, and combine results for exclusive decays to
left-handed etau (\mu tau) pairs. We set an $H^{\pm\pm}$
lower mass limit of 114(112) GeV/c2 at the 95% confidence
level.},
Doi = {10.1103/physrevlett.101.121801},
Key = {fds308579}
}
@article{fds308584,
Author = {Aaltonen, and T, and others},
Title = {{Search for Heavy Top-like Quarks Using Lepton Plus Jets
Events in 1.96-TeV $p \bar{p}$ Collisions}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {16},
Pages = {161803},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.161803},
Abstract = {We present the results of a search for pair production of a
new heavy toplike quark t[prime] decaying to a ${W}$ boson
and another quark using the Collider Detector at Fermilab II
detector in run II of the Tevatron $p\bar{p}$ collider.
Using a data sample corresponding to 760 pb-1 of integrated
luminosity, we fit the observed spectrum of total transverse
energy and reconstructed t[prime] quark mass to a
combination of standard model processes and t[prime] pair
production. We see no evidence for t[prime][overline
t][prime] production, and we infer a lower limit of 256
GeV/c2 on the mass of the t[prime] at 95% C.L. assuming
standard strong couplings for the t[prime].},
Doi = {10.1103/physrevlett.100.161803},
Key = {fds308584}
}
@article{fds308611,
Author = {Aaltonen, and T, and others},
Title = {{Search for Heavy, Long-Lived Neutralinos that Decay to
Photons at CDF II Using Photon Timing}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {3},
Pages = {032015},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.032015},
Abstract = {We present the results of the first hadron collider search
for heavy, long-lived neutralinos that decay via
chi-tilde10-->gammaG-tilde in gauge-mediated supersymmetry
breaking models. Using an integrated luminosity of 570\pm 34
pb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV, we
select gamma+jet+missing transverse energy candidate events
based on the arrival time of a high-energy photon at the
electromagnetic calorimeter as measured with a timing system
that was recently installed on the CDF II detector. We find
2 events, consistent with the background estimate of 1.3\pm
0.7 events. While our search strategy does not rely on
model-specific dynamics, we set cross section limits and
place the world-best 95% C.L. lower limit on the chi-tilde10
mass of 101 GeV/c2 at tauchi-tilde[sub 1][sup 0]=5
ns.},
Doi = {10.1103/PhysRevD.78.032015},
Key = {fds308611}
}
@article{fds308578,
Author = {Aaltonen, and T, and others},
Title = {{Search for large extra dimensions in final states
containing one photon or jet and large missing transverse
energy produced in $p \bar{p}$ collisions at $\sqrt{s}$ =
1.96-TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {101},
Number = {18},
Pages = {181602},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.181602},
Abstract = {We present the results of searches for large extra
dimensions in samples of events with large missing
transverse energy E-slash T and either a photon or a jet
produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
collected with the Collider Detector at Fermilab II. For
gamma+E-slash T and jet+E-slash T candidate samples
corresponding to 2.0 and 1.1 fb-1 of integrated luminosity,
respectively, we observe good agreement with standard model
expectations and obtain a combined lower limit on the
fundamental parameter of the large extra dimensions model MD
as a function of the number of extra dimensions in the
model.},
Doi = {10.1103/physrevlett.101.181602},
Key = {fds308578}
}
@article{fds308602,
Author = {Aaltonen, and T, and others},
Title = {{Search for New Heavy Particles Decaying to $Z^0 Z^0 \to
eeee$ in $p$ - $\bar{p}$ Collisions at $\sqrt{s}$ = 1.96-
TeV}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {1},
Pages = {012008},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.012008},
Abstract = {We report the results of a search for the anomalous
production of a massive particle decaying to four electrons
via two Z0 bosons in 1.1 fb-1 of $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV collected by the CDF II detector at
Fermilab. We employ optimized electron identification
criteria to maximize acceptance and efficiency. We estimate
the backgrounds in the invariant mass range 500–1000
GeV/c2 to be 0.028\pm 0.009(stat)\pm 0.011(syst) events. We
observe zero events in this search region. Assuming a
Randall-Sundrum graviton production model, we set 95% C.L.
limits on sigma×BF(G-->Z0Z0)},
Doi = {10.1103/PhysRevD.78.012008},
Key = {fds308602}
}
@article{fds308580,
Author = {Aaltonen, and T, and others},
Title = {{Search for Pair Production of Scalar Top Quarks Decaying to
a $\tau$ Lepton and a $b$ Quark in $p\bar{p}$ Collisions at
sqrt{s}=1.96 TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {101},
Number = {7},
Pages = {071802},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.071802},
Abstract = {We search for pair production of supersymmetric top quarks
(t-tilde1), followed by R-parity violating decay
t-tilde1-->taub with a branching ratio beta, using 322 pb-1
of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV collected by
the upgraded Collider Detector at Fermilab. Two candidate
events pass our final selection criteria, consistent with
the standard model expectation. We set upper limits on the
cross section sigma(t-tilde1[overline t-tilde ]1)×beta2 as
a function of the top-squark mass m(t-tilde1). Assuming
beta=1, we set a 95% confidence level limit m(t-tilde1)>153
GeV/c2. The limits are also applicable to the case of a
third-generation scalar leptoquark (LQ3) decaying
LQ3-->taub.},
Doi = {10.1103/physrevlett.101.071802},
Key = {fds308580}
}
@article{fds308597,
Author = {Aaltonen, and T, and others},
Title = {{Search for resonant $t \bar{t}$ production in $p \bar{p}$
collisions at $\sqrt{s}$ = 1.96-TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {23},
Pages = {231801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.231801},
Abstract = {We report on a search for narrow-width particles decaying to
a top and antitop quark pair. The data set used in the
analysis corresponds to an integrated luminosity of 680 pb-1
collected with the Collider Detector at Fermilab in run II.
We present 95% confidence level upper limits on the cross
section times branching ratio. Assuming a specific
top-color-assisted technicolor production model, the
leptophobic Z[prime] with width GammaZ[prime]=0.012MZ[prime],
we exclude the mass range MZ[prime]},
Doi = {10.1103/physrevlett.100.231801},
Key = {fds308597}
}
@article{fds308592,
Author = {Aaltonen, and T, and others},
Title = {{Search for Standard Model Higgs Bosons Produced in
Association with ${W}$ Bosons}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {4},
Pages = {041801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.041801},
Abstract = {We report the observation of two narrow resonances
consistent with states of orbitally excited (L=1) Bs mesons
using 1 fb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
collected with the Collider Detector at Fermilab II detector
at the Fermilab Tevatron. We use two-body decays into K- and
B+ mesons reconstructed as B+-->J/psiK+, J/psi-->\mu +\mu -
or B+-->[overline D]0pi+, [overline D]0-->K+pi-. We deduce
the masses of the two states to be m(Bs1)=5829.4\pm 0.7
MeV/c2 and m(Bs2*)=5839.6\pm 0.7 MeV/c2.},
Doi = {10.1103/physrevlett.100.041801},
Key = {fds308592}
}
@article{fds308581,
Author = {Aaltonen, and T, and others},
Title = {{Search for the Higgs boson in events with missing
transverse energy and $b$ quark jets produced in proton-
antiproton collisions at $\sqrt{s}$ =1.96
TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {21},
Pages = {211801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.211801},
Abstract = {We search for the standard model Higgs boson produced in
association with an electroweak vector boson in events with
no identified charged leptons, large imbalance in transverse
momentum, and two jets where at least one contains a
secondary vertex consistent with the decay of b hadrons. We
use ~1 fb-1 integrated luminosity of $p\bar{p}$ collisions
at $\sqrt{s}=1.96$ TeV recorded by the Collider Detector at
Fermilab II experiment at the Tevatron. We find 268 (16)
single (double) b-tagged candidate events, where $248\pm 43$
($14.4\pm 2.7$) are expected from standard model background
processes. We observe no significant excess over the
expected background and thus set 95% confidence level upper
limits on the Higgs boson production cross section for
several Higgs boson masses ranging from 110 to 140 GeV/c2.
For a mass of 115 GeV/c2, the observed (expected) limit is
20.4 (14.2) times the standard model prediction.},
Doi = {10.1103/physrevlett.100.211801},
Key = {fds308581}
}
@article{fds308594,
Author = {Aaltonen, and T, and others},
Title = {{Search for third generation vector leptoquarks in
$p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96-TeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {9},
Pages = {091105},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.091105},
Abstract = {We search for a third generation vector leptoquark (VLQ3)
that decays to a $b$ quark and tau lepton using the CDF II
detector and 320 pb-1 of integrated luminosity from the
Fermilab Tevatron. Observing a number of events in agreement
with standard model expectations, we obtain, assuming
Yang-Mills (minimal) couplings, the most stringent upper
limit on the VLQ3 pair production cross section of 344 fb
(493 fb) and lower limit on the VLQ3 mass of 317 GeV/c2 (251
GeV/c2) at 95% C.L.},
Doi = {10.1103/PhysRevD.77.091105},
Key = {fds308594}
}
@article{fds308582,
Author = {Aaltonen, and T, and others},
Title = {{Strong Evidence for $Z Z$ Production in panti-p Collisions
at $\sqrt{s}$ = 1.96-TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {20},
Pages = {201801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.201801},
Abstract = {We report the first evidence of Z boson pair production at a
hadron collider with a significance exceeding 4 standard
deviations. This result is based on a data sample
corresponding to 1.9 fb-1 of integrated luminosity from
$p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV collected with
the Collider Detector at Fermilab II detector. In the
[script-l][script-l][script-l][prime][script-l][prime]
channel, we observe three ZZ candidates with an expected
background of 0.096-0.063+0.092 events. In the
[script-l][script-l]nunu channel, we use a leading-order
calculation of the relative ZZ and WW event probabilities to
discriminate between signal and background. In the
combination of [script-l][script-l][script-l][prime][script-l][prime]
and [script-l][script-l]nunu channels, we observe an excess
of events with a probability of 5.1×10-6 to be due to the
expected background. This corresponds to a significance of
4.4 standard deviations. The measured cross section is
sigma($p\bar{p}$-->ZZ)=1.4-0.6+0.7(stat+syst) pb, consistent
with the standard model expectation.},
Doi = {10.1103/physrevlett.100.201801},
Key = {fds308582}
}
@article{fds308606,
Author = {Aaltonen, and T, and others},
Title = {{Two-particle momentum correlations in jets produced in $p
\bar{p}$ Collisions at $\sqrt{s}$ = 1.96-TeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {9},
Pages = {092001},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.092001},
Abstract = {We present the first measurement of two-particle momentum
correlations in jets produced in $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV. Results are obtained for charged
particles within a restricted cone with an opening angle of
0.5 radians around the jet axis and for events with dijet
masses between 66 and 563 GeV/c2. A comparison of the
experimental data to theoretical predictions obtained for
partons within the framework of resummed perturbative QCD in
the next-to-leading log approximation shows that the parton
momentum correlations survive the hadronization stage of jet
fragmentation, giving further support to the hypothesis of
local parton-hadron duality. The extracted value of the
next-to-leading-log-approximation parton shower cutoff scale
Qeff set equal to LambdaQCD is found to be
(1.4-0.7+0.9)×100 MeV.},
Doi = {10.1103/PhysRevD.77.092001},
Key = {fds308606}
}
%% Papers Submitted
@article{fds375132,
Author = {M.C. Kruse and ATLAS collaboration},
Title = {Search for top-philic heavy resonances in $pp$ collisions at
$\sqrt{s}=13$ TeV with the ATLAS detector},
Journal = {EPJC},
Year = {2023},
Month = {April},
url = {https://arxiv.org/abs/2304.01678},
Abstract = {https://arxiv.org/abs/2304.01678},
Key = {fds375132}
}
@article{fds225756,
Author = {K. Finelli and M.C. Kruse and A. Limosani and A. Saavedra (ATLAS
collaboration)},
Title = {Simultaneous measurements of the tt¯, W+W−, and
Z/γ∗→ττ production cross-sections in pp collisions at
s√=7 TeV with the ATLAS detector},
Journal = {PRD},
Year = {2014},
url = {http://arxiv.org/abs/1407.0573},
Abstract = {http://arxiv.org/abs/1407.0573},
Key = {fds225756}
}
%% Preprints
@article{fds4629,
Author = {M.C. Kruse},
Title = {The Silicon tracking upgrade at CDF},
Publisher = {FERMILAB-CONF-98-109-E},
Year = {1998},
Month = {January},
url = {http://www-lib.fnal.gov/archive/1998/conf/Conf-98-109-E.html},
Abstract = {http://www-lib.fnal.gov/archive/1998/conf/Conf-98-109-E.html},
Key = {fds4629}
}