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Measurement of the Z/gamma* + b-jet cross section in pp collisions at 7 TeV

Author: Abbaneo D.
Abbiendi G.
Abbrescia M.
Abdullin S.
Acosta D.
Acosta J. G.
Acosta M. Vazquez
Adair A.
Adam N.
Adam W.
Adams M. R.
Adams T.
Adiguzel A.
Adler V.
Adzic P.
Afanasiev S.
Agostino L.
Agram J-L
Aguilar-Benitez M.
Aguilo E.
Ahmad M.
Ahmad W. Haj
Ahuja S.
Akchurin N.
Akgun B.
Akgun U.
Akin I. V.
Alagoz E.
Albajar C.
Albayrak E. A.
Albergo S.
Albrow M.
Alcaraz Maestre J.
Alda Junior W. L.
Alexander J.
Aliev T.
Almeida N.
Alver B.
Alverson G.
Alves G. A.
Amapane N.
Amsler C.
Anagnostou G.
Anastassov A.
Anderson J.
Anderson M.
Andrea J.
Andreev V.
Andreev V.
Andreev Yu.
Andrews W.
Anghel I. M.
Anjos T. S.
Antonelli L.
Antunes J. Rodrigues
Antunovic Z.
Apanasevich L.
Apollinari G.
Appelt E.
Apresyan A.
Aranyi A.
Arce P.
Arcidiacono R.
Arenton M. W.
Arfaei H.
Argiro S.
Arisaka K.
Arneodo M.
Arora S.
Asawatangtrakuldee C.
Asghar M. I.
Askew A.
Assran Y.
Ata M.
Atac M.
Atramentov O.
Attikis A.
Auffray E.
Autermann C.
Auzinger G.
Avdeeva E.
Avery P.
Avetisyan A.
Azarkin M.
Azhgirey I.
Aziz T.
Azzi P.
Azzolini V.
Azzurri P.
Baarmand M. M.
Babb J.
Bacchetta N.
Bachtis M.
Baden A.
Baeni L.
Baesso P.
Baffioni S.
Bagliesi G.
Bai Y.
Baillon P.
Bainbridge R.
Bakhshiansohi H.
Bakirci M. N.
Bakken J. A.
Balazs M.
Ball A. H.
Ball G.
Ban Y.
Banerjee S.
Banerjee S.
Bansal S.
Banzuzi K.
Barbagli G.
Barberis E.
Barbone L.
Bardak C.
Barfuss A. F.
Bargassa P.
Barge D.
Baringer P.
Barker A.
Barnes V. E.
Barnett B. A.
Barney D.
Barone L.
Barrett M.
Bartalini P.
Barth C.
Basegmez S.
Basso L.
Battilana C.
Baty C.
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Baumgartel D.
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Belyaev A.
Benaglia A.
Bencze G.
Bendavid J.
Benedetti D.
Benelli G.
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Wood J.
Wood J. S.
Worm S. D.
Wright D.
Wrochna G.
Wu W.
Wuerthwein F.
Wulz C-E
Wyslouch B.
Xiao H.
Xie S.
Xu M.
Yagil A.
Yalvac M.
Yang F.
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Yang Z. C.
Yazgan E.
Yelton J.
Yetkin T.
Yi K.
Yildirim E.
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Yohay R.
Yoo H. D.
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Yun J. C.
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Zakaria M.
Zalewski P.
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Zarubin A.
Zatserklyaniy A.
Zeinali M.
Zeise M.
Zeuner W. D.
Zeyrek M.
Zhang J.
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Zheng Y.
Zhokin A.
Zhu B.
Zhu R. Y.
Zhukov V.
Zhukova V.
Ziebarth E. B.
Ziegler J.
Zielinski M.
Zito G.
Zoeller M. H.
Zotto P.
Zou W.
Zumerle G.
Zuranski A.
Publication venue: 'Springer Science and Business Media LLC'
Publication date: 01/01/2012
Field of study

The production of b jets in association with a Z/gamma* boson is studied using proton-proton collisions delivered by the LHC at a centre-of-mass energy of 7 TeV and recorded by the CMS detector. The inclusive cross section for Z/gamma* + b-jet production is measured in a sample corresponding to an integrated luminosity of 2.2 inverse femtobarns. The Z/gamma* + b-jet cross section with Z/gamma* to ll (where ll = ee or mu mu) for events with the invariant mass 60 < M(ll) < 120 GeV, at least one b jet at the hadron level with pT > 25 GeV and abs(eta) < 2.1, and a separation between the leptons and the jets of Delta R > 0.5 is found to be 5.84 +/- 0.08 (stat.) +/- 0.72 (syst.) +(0.25)/-(0.55) (theory) pb. The kinematic properties of the events are also studied and found to be in agreement with the predictions made by the MadGraph event generator with the parton shower and the hadronisation performed by PYTHIA.Comment: Submitted to the Journal of High Energy Physic

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Constraints on the χ_(c1) versus χ_(c2) polarizations in proton-proton collisions at √s = 8 TeV

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Abbiendi G.
Abbrescia M.
Abdullin S.
Abercrombie D.
Acharya H.
Acosta D.
Acosta J. G.
Adam W.
Adams M. R.
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Adzic P.
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Wulz C.-E.
Wyslouch B.
Wöhri H. K.
Wöhrmann C.
Würthwein F.
Xia F.
Xiao M.
Xiao R.
Xie S.
Xie W.
Yagil A.
Yalvac M.
Yang U.K.
Yang Y. C.
Yates B. R.
Yazgan E.
Yetkin E. A.
Yi K.
Yohay R.
Yoo H. D.
Yoo J.
Yoon I.
Yu D.
Yu G. B.
Yu I.
Yu S. S.
Yuan L.
Yumiceva F.
Yusli M. N.
Zabi A.
Zacharopoulou A.
Zahid S.
Zaleski S.
Zalewski P.
Zanetti A.
Zanetti M.
Zarubin A.
Zarucki M.
Zecchinelli A. G.
Zenaiev O.
Zenz S. C.
Zeuner W. D.
Zevi Della Porta G.
Zghiche A.
Zhang A.
Zhang F.
Zhang H.
Zhang J.
Zhang S.
Zhang W.
Zhang Y.
Zhang Z.
Zhao J.
Zhokin A.
Zhu D. H.
Zhu R. Y.
Zientek M.
Zlebcik R.
Zobec J.
Zoi I.
Zolkapli Z.
Zorbakir I. S.
Zorbilmez C.
Zotto P.
Zou D.
Zucchetta A.
Zumerle G.
Zuo X.
Zuolo D.
Álvarez Fernández A.
Özçelik Ö.
Publication venue: 'American Physical Society (APS)'
Publication date: 24/04/2020
Field of study

The polarizations of promptly produced χ_(c1) and χ_(c2) mesons are studied using data collected by the CMS experiment at the LHC, in proton-proton collisions at √s=8 TeV. The χ_c states are reconstructed via their radiative decays χ_c → J/ψγ, with the photons being measured through conversions to e⁺e⁻, which allows the two states to be well resolved. The polarizations are measured in the helicity frame, through the analysis of the χ_(c2) to χ_(c1) yield ratio as a function of the polar or azimuthal angle of the positive muon emitted in the J/ψ → μ⁺μ⁻ decay, in three bins of J/ψ transverse momentum. While no differences are seen between the two states in terms of azimuthal decay angle distributions, they are observed to have significantly different polar anisotropies. The measurement favors a scenario where at least one of the two states is strongly polarized along the helicity quantization axis, in agreement with nonrelativistic quantum chromodynamics predictions. This is the first measurement of significantly polarized quarkonia produced at high transverse momentum

Caltech Authors

Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy

Author: Abbaneo D
Abbiendi G
Abbrescia M
Abdullin S
Abdulsalam A
Acosta D
Acosta JG
Adair A
Adam N
Adam W
Adams JR
Adams MR
Adams T
Adiguzel A
Adler V
Adzic P
Agram JL
Aguilar-Benitez M
Aguilo E
Ahmad M
Ahmad WH
Ahuja S
Akchurin N
Akgun B
Akgun U
Akin IV
Alagoz E
Albajar C
Albayrak EA
Albergo S
Albrow M
Alcaraz Maestre J
Alda Junior WL
Aldaya Martin M
Alexander J
Aliev T
Alimena J
Almeida N
Alverson G
Alves GA
Amapane N
Amsler C
Anagnostou G
Anastassov A
Anderson J
Anderson M
Andrea J
Andreev V
Andreev V
Andreev Y
Andrews W
Anghel IM
Antonelli L
Antunovic Z
Apanasevich L
Appelt E
Apresyan A
Arce P
Arcidiacono R
Arenton MW
Arfaei H
Argiro S
Arneodo M
Arora S
Asawatangtrakuldee C
Asghar MI
Askew A
Assran Y
Ata M
Attikis A
Auffray E
Autermann C
Auzinger G
Avdeeva E
Avery P
Avetisyan A
Avila C
Azarkin M
Azhgirey I
Aziz T
Azzi P
Azzolini V
Azzurri P
Baarmand MM
Babb J
Bacchetta N
Bachtis M
Baden A
Baeni L
Baffioni S
Bagliesi G
Bai Y
Baillon P
Bainbridge R
Bakhshiansohi H
Bakirci MN
Balazs M
Ball AH
Ball G
Ban Y
Banerjee S
Banerjee S
Bansal S
Banzuzi K
Barbagli G
Barberis E
Barbone L
Barfuss AF
Bargassa P
Barge D
Baringer P
Barker A
Barnes VE
Barnett BA
Barney D
Barone L
Bartalini P
Barth C
Basegmez S
Basso L
Battilana C
Bauer G
Bauerdick LAT
Baumgartel D
Baur U
Bayshev I
Bazterra VE
Bean A
Beauceron S
Beaudette F
Beaupere N
Beernaert K
Behr J
Behrenhoff W
Behrens U
Belforte S
Beliy N
Belknap D
Bell AJ
Bell KW
Bellan P
Bellan R
Belotelov I
Belyaev A
Belyaev A
Benaglia A
Bencze G
Bendavid J
Benedetti D
Benelli G
Benhabib L
Beni N
Benussi L
Benvenuti AC
Beranek S
Beretvas A
Bergauer T
Berger J
Bergholz M
Beri SB
Bernardes CA
Bernet C
Berry D
Berry E
Berryhill J
Bertl W
Besancon M
Betchart B
Bethani A
Betts RR
Beuselinck R
Bhardwaj A
Bhat PC
Bhatnagar V
Bhattacharya S
Bhattacharya S
Bhatti A
Bialkowska H
Bian JG
Bianchi G
Bianchini L
Bianco S
Biasini M
Biino C
Bilei GM
Bilin B
Bilinskas MJ
Bilki B
Bilmis S
Bitioukov S
Blekman F
Blobel V
Bloch D
Bloch I
Bloch P
Bloom K
Bluj M
Blumenfeld B
Blyweert S
Bobrovskyi S
Boccali T
Bocci A
Bochenek J
Bodek A
Bodin D
Boeser C
Boimska B
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Bondu O
Bontenackels M
Boos E
Bornheim A
Borras K
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Bostock F
Botta C
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Boulahouache C
Bourilkov D
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Braibant-Giacomelli S
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Branson JG
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Brochero Cifuentes JA
Brom JM
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Bucinskaite I
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Carrillo Montoya CA
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Castaldi R
Castello R
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Castro A
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Caudron A
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Cavallari F
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Cavallo N
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Ceard L
Cepeda M
Cerati GB
Cerci DS
Cerci S
Cerizza G
Cerminara G
Cerrada M
Chabert EC
Chadwick M
Chakaberia I
Chamizo Llatas M
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Chang P
Chang S
Chang YH
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Charaf O
Charlot C
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Chatrchyan S
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Chauhan S
Checchia P
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Cheung HWK
Chhibra SS
Chierici R
Chiochia V
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Chlebana F
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CMS Collaboration
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Cockerill DJA
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D'Enterria D
D'Hondt J
Da Costa EM
Dabrowski A
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Damgov J
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Dammann D
Danielson T
Das S
Daskalakis G
Dasu S
Daubie E
Dauncey P
David A
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de Barbaro P
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De Boer W
De Cosa A
de Fatis TT
De Filippis N
De Gruttola M
De Guio F
De La Barca Sanchez MC
De La Cruz B
De La Cruz-Burelo E
De Lentdecker G
De Mattia M
de Monchenault GH
De Oliveira Martins C
De Palma M
De Roeck A
de Troconiz JF
De Visscher S
De Wolf EA
Deisher A
Deiters K
Dejardin M
Del Re D
Delaere C
Delgado Peris A
Dell'Orso R
Della Negra M
Della Ricca G
Demaria N
Demina R
Demortier L
Denegri D
Deniz M
Depasse P
Dermenev A
Dero V
Descroix A
Dhingra N
Di Giovanni GP
Di Guida S
Di Marco E
Di Matteo L
Diamond B
Dias FA
Diemoz M
Dierlamm A
Dietz C
Dietz-Laursonn E
Diez Pardos C
Dimitrov A
Dinardo ME
Dissertori G
Dittmar M
Djordjevic M
Dobrzynski L
Dobson M
Dobur D
Doesburg R
Dogangun O
Dolen J
Dominguez Vazquez D
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Don CKK
Dorigo T
Dorney B
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Dragoiu C
Drell BR
Dremin I
Drouhin F
Drozdetskiy A
du Pree T
Duarte Campderros J
Duarte J
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Elliott-Peisert A
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Faure JL
Favaro C
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Ferapontov A
Ferencek D
Ferguson T
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Fernandes M
Fernandez Bedoya C
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Fernandez Perez Tomei TR
Fernandez Ramos JP
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Ferreira Parracho PG
Ferri F
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Field RD
Finger M
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Fiore L
Fiorendi S
Fiori F
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Fisk I
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Geurts FJM
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Zito G
Zou W
Zucchetta A
Zumerle G
Zuranski A
Publication venue: 'American Physical Society (APS)'
Publication date: 01/01/2012
Field of study

A search for new physics is performed in events with two same-sign isolated leptons, hadronic jets, and missing transverse energy in the final state. The analysis is based on a data sample corresponding to an integrated luminosity of 4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of 7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of 140 increase in integrated luminosity over previously published results. The observed yields agree with the standard model predictions and thus no evidence for new physics is found. The observations are used to set upper limits on possible new physics contributions and to constrain supersymmetric models. To facilitate the interpretation of the data in a broader range of new physics scenarios, information on the event selection, detector response, and efficiencies is provided.Comment: Published in Physical Review Letter

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Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV

Author: Abbaneo D
Abbiendi G
Abbrescia M
Abdullin S
Abdulsalam A
Acosta D
Acosta JG
Acosta MV
Adair A
Adam N
Adam W
Adams MR
Adams T
Adiguzel A
Adler V
Adzic P
Afanasiev S
Agostino L
Agram JL
Aguilar-Benitez M
Aguilo E
Ahmad M
Ahmad WH
Ahuja S
Akchurin N
Akgun B
Akgun U
Akin IV
Alagoz E
Albajar C
Albayrak EA
Albergo S
Albrow M
Alcaraz Maestre J
Alda Junior WL
Alexander J
Aliev T
Alimena J
Almeida N
Alverson G
Alves GA
Amapane N
Amsler C
Anagnostou G
Anastassov A
Anderson J
Anderson M
Andrea J
Andreev V
Andreev V
Andreev Y
Andrews W
Anghel IM
Anjos TS
Antonelli L
Antunovic Z
Apanasevich L
Appelt E
Apresyan A
Arce P
Arcidiacono R
Arenton MW
Arfaei H
Argiro S
Arneodo M
Arora S
Asawatangtrakuldee C
Asghar MI
Askew A
Assran Y
Ata M
Attikis A
Auffray E
Autermann C
Auzinger G
Avdeeva E
Avery P
Avetisyan A
Avila C
Azarkin M
Azhgirey I
Aziz T
Azzi P
Azzolini V
Azzurri P
Baarmand MM
Babb J
Bacchetta N
Bachtis M
Baden A
Baeni L
Baffioni S
Bagliesi G
Bai Y
Baillon P
Bainbridge R
Bakhshiansohi H
Bakirci MN
Balazs M
Ball AH
Ball G
Ban Y
Banerjee S
Banerjee S
Bansal S
Banzuzi K
Barbagli G
Barberis E
Barbone L
Barfuss AF
Bargassa P
Barge D
Baringer P
Barker A
Barnes VE
Barnett BA
Barney D
Barone L
Barrett M
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Publication venue: 'American Physical Society (APS)'
Publication date: 01/01/2012
Field of study

The azimuthal anisotropy of charged particles in PbPb collisions at nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS detector at the LHC over an extended transverse momentum (pt) range up to approximately 60 GeV. The data cover both the low-pt region associated with hydrodynamic flow phenomena and the high-pt region where the anisotropies may reflect the path-length dependence of parton energy loss in the created medium. The anisotropy parameter (v2) of the particles is extracted by correlating charged tracks with respect to the event-plane reconstructed by using the energy deposited in forward-angle calorimeters. For the six bins of collision centrality studied, spanning the range of 0-60% most-central events, the observed v2 values are found to first increase with pt, reaching a maximum around pt = 3 GeV, and then to gradually decrease to almost zero, with the decline persisting up to at least pt = 40 GeV over the full centrality range measured.Comment: Replaced with published version. Added journal reference and DO

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Compressed representation of a partially defined integer function over multiple arguments

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Abbiendi G
Abbrescia M
Abdelalim AA
Abdullin S
Abdulsalam A
Acosta D
Acosta MV
Adair A
Adam W
Adams MR
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Adiguzel A
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Aguilar-Benitez M
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Publication venue
Publication date: 01/01/2013
Field of study

In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one

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Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV

Author: Abbaneo D
Abbiendi G
Abbrescia M
Abdullin S
Abdulsalam A
Acosta D
Acosta JG
Acosta MV
Adair A
Adam N
Adam W
Adams JR
Adams MR
Adams T
Adiguzel A
Adler V
Adzic P
Afanasiev S
Agram JL
Aguilar-Benitez M
Aguilo E
Ahmad M
Ahmad WH
Ahuja S
Akchurin N
Akgun B
Akgun U
Akin IV
Alagoz E
Albajar C
Albayrak EA
Albergo S
Albrow M
Alcaraz Maestre J
Alda Junior WL
Alexander J
Aliev T
Alimena J
Almeida N
Alverson G
Alves GA
Amapane N
Amsler C
Anagnostou G
Anastassov A
Anderson J
Anderson M
Andrea J
Andreev V
Andreev V
Andreev Y
Andrews W
Anghel IM
Antonelli L
Antunes JR
Antunovic Z
Apanasevich L
Appelt E
Apresyan A
Arce P
Arcidiacono R
Arenton MW
Arfaei H
Argiro S
Arneodo M
Arora S
Asawatangtrakuldee C
Asghar MI
Askew A
Assran Y
Ata M
Attikis A
Auffray E
Autermann C
Auzinger G
Avdeeva E
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Avetisyan A
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Azhgirey I
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Azzolini V
Azzurri P
Baarmand MM
Babb J
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Baden A
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Baffioni S
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Bakhshiansohi H
Bakirci MN
Balazs M
Ball AH
Ball G
Ban Y
Banerjee S
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Bansal S
Banzuzi K
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Barfuss AF
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Barnes VE
Barnett BA
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Basegmez S
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Battilana C
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Bauerdick LAT
Baumgartel D
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Bayshev I
Bazterra VE
Bean A
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Beaudette F
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de Monchenault GH
De Oliveira Martins C
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de Troconiz JF
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De Wolf EA
Deisher A
Deiters K
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del Arbol PMR
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Denegri D
Deniz M
Depasse P
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Dero V
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Di Giovanni GP
Di Guida S
Di Marco E
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Diamond B
Dias FA
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Dimitrov A
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Zuranski A
Publication venue: 'Springer Science and Business Media LLC'
Publication date: 01/01/2012
Field of study

Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of 2.76 TeV per nucleon pair was studied using data collected with the CMS detector at the LHC. Fragmentation functions are constructed using charged-particle tracks with transverse momenta pt > 4 GeV for dijet events with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events are compared to those in pp data as a function of collision centrality, as well as dijet-pt imbalance. Special emphasis is placed on the most central PbPb events including dijets with unbalanced momentum, indicative of energy loss of the hard scattered parent partons. The fragmentation patterns for both the leading and subleading jets in PbPb collisions agree with those seen in pp data at 2.76 TeV. The results provide evidence that, despite the large parton energy loss observed in PbPb collisions, the partition of the remaining momentum within the jet cone into high-pt particles is not strongly modified in comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic

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Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV

Author: Abbaneo D
Abbiendi G
Abbrescia M
Abdullin S
Acosta D
Acosta JG
Acosta MV
Adair A
Adam N
Adam W
Adams MR
Adams T
Adiguzel A
Adler V
Adzic P
Agostino L
Agram JL
Aguilar-Benitez M
Aguilo E
Ahmad M
Ahmad WH
Ahuja S
Akchurin N
Akgun B
Akgun U
Akin IV
Alagoz E
Albajar C
Albayrak EA
Albergo S
Albrow M
Alda Junior WL
Alexander J
Aliev T
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Sfiligoi I
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Publication venue: 'IOP Publishing'
Publication date: 01/01/2012
Field of study

The performance of muon reconstruction, identification, and triggering in CMS has been studied using 40 inverse picobarns of data collected in pp collisions at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection criteria covering a wide range of physics analysis needs have been examined. For all considered selections, the efficiency to reconstruct and identify a muon with a transverse momentum pT larger than a few GeV is above 95% over the whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4, while the probability to misidentify a hadron as a muon is well below 1%. The efficiency to trigger on single muons with pT above a few GeV is higher than 90% over the full eta range, and typically substantially better. The overall momentum scale is measured to a precision of 0.2% with muons from Z decays. The transverse momentum resolution varies from 1% to 6% depending on pseudorapidity for muons with pT below 100 GeV and, using cosmic rays, it is shown to be better than 10% in the central region up to pT = 1 TeV. Observed distributions of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO

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