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Measurement of the top-quark mass in tt¯ events with dilepton final states in pp collisions at √s = 7 TeV

Author: Abbaneo D.
Abbiendi G.
Abbrescia M.
Abdullin S.
Abdulsalam A.
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.
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.
AldaJunior W. L.
Alexander J.
Aliev T.
Alimena J.
Almeida N.
Alverson G.
Alves A.
Alves G. A.
Amapane N.
Amsler C.
Anagnostou G.
Anastassov A.
Anderson J.
Anderson M.
Andrea J.
Andreev V.
Andreev V.
Andreev Y.u.
Andrews W.
Anghel I. M.
Anh TV
Anjos T. S.
Ansari M. H.
Antonelli L.
Antunes J. Rodrigues
Antunovic Z.
Apanasevich L.
Appelt E.
Apresyan A.
Apyan A.
Arce P.
Arcidiacono R.
Arenton M. W.
Arfaei H.
Argiro S.
Arneodo M.
Arora S.
Asawatangtrakuldee C.
Asghar M. I.
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 M. M.
Babb J.
Bacchetta N.
Bachtis M.
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Baeni L.
Baffioni S.
Bagliesi G.
Bai Y.
Baillon P.
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Bakirci M. N.
Balazs M.
Ball A. H.
Ball G.
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Banerjee S.
Bansal M.
Bansal S.
Banzuzi K.
Barbagli G.
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Basegmez S.
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MESSINEO ALBERTO MARIA
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Publication venue: 'Springer Science and Business Media LLC'
Publication date: 01/01/2012
Field of study

Open Access: This article is distributed under the terms of the Creative Commons Attribution License.-- Chatrchyan, S. et al.The top-quark mass is measured in proton-proton collisions at s√=7 TeV using a data sample corresponding to an integrated luminosity of 5.0 fb−1 collected by the CMS experiment at the LHC. The measurement is performed in the dilepton decay channel tt¯→(ℓ+νℓb)(ℓ−ν¯¯ℓb¯), where ℓ=e,μ. Candidate top-quark decays are selected by requiring two leptons, at least two jets, and imbalance in transverse momentum. The mass is reconstructed with an analytical matrix weighting technique using distributions derived from simulated samples. Using a maximum-likelihood fit, the top-quark mass is determined to be 172.5±0.4 (stat.)±1.5 (syst.) GeV.Acknowledge support from BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); MoER, SF0690030s09 and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France);BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); MSI (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MON, RosAtom, RAS and RFBR (Russia); MSTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); ThEP, IPST and NECTEC (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA). Individuals have received support from the Marie-Curie program and the European Research Council (European Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander von Humboldt Foundation; the Austrian Science Fund (FWF); the Belgian Federal Science Policy Office; the Fonds pour la Formation à la Recherche dans l’Industrie et dans l’Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWTBelgium); the Ministry of Education, Youth and Sports (MEYS) of Czech Republic; the Council of Science and Industrial Research, India; the Compagnia di San Paolo (Torino); and the HOMING PLUS program of Foundation for Polish Science, cofinanced from European Union, Regional Development Fund.Peer Reviewe

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Measurement of the production cross section ratio σ(χb2(1P))/σ(χb1(1P))in pp collisions at √s=8TeV

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Abbrescia M
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Adiguzel A
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Asawatangtrakuldee C
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Zuranski A
Publication venue: Elsevier
Publication date: 01/01/2014
Field of study

A measurement of the production cross section ratio σ(χb2(1P))/σ(χb1(1P))σ(χb2(1P))/σ(χb1(1P)) is presented. The χb1(1P)χb1(1P) and χb2(1P)χb2(1P) bottomonium states, promptly produced in pp collisions at View the MathML sources=8 TeV, are detected by the CMS experiment at the CERN LHC through their radiative decays χb1,2(1P)→ϒ(1S)+γχb1,2(1P)→ϒ(1S)+γ. The emitted photons are measured through their conversion to e+e−e+e− pairs, whose reconstruction allows the two states to be resolved. The ϒ(1S)ϒ(1S) is measured through its decay to two muons. An event sample corresponding to an integrated luminosity of 20.7 fb−120.7 fb−1 is used to measure the cross section ratio in a phase-space region defined by the photon pseudorapidity, |ηγ|<1.0|ηγ|<1.0; the ϒ(1S)ϒ(1S) rapidity, |yϒ|<1.5|yϒ|<1.5; and the ϒ(1S)ϒ(1S) transverse momentum, View the MathML source7<pTϒ<40 GeV. The cross section ratio shows no significant dependence on the ϒ(1S)ϒ(1S) transverse momentum, with a measured average value of View the MathML source0.85±0.07(stat+syst)±0.08(BF), where the first uncertainty is the combination of the experimental statistical and systematic uncertainties and the second is from the uncertainty in the ratio of the χbχb branching fractions

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Searches for new physics using the t(t)over-bar invariant mass distribution in pp collisions at √s=8 TeV

Author: Abbaneo D
Abbiendi G
Abbrescia M
Abdelalim AA
Abdullin S
Abdulsalam A
Acosta D
Acosta JG
Acosta MV
Adair A
Adam W
Adams MR
Adams T
Adiguzel A
Adler V
Adzic P
Afanasiev S
Agram J-L
Aguilar-Benitez M
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
Alderweireldt S
Alexander J
Aliev T
Alimena J
Almeida N
Alverson G
Alves GA
Amapane N
Amsler C
Anagnostou G
Anastassov A
Anderson J
Andrea J
Andreev V
Andreev V
Andreev Y
Andrews W
Androsov K
Antonelli L
Antunovic Z
Apanasevich L
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Publication venue: 'American Physical Society (APS)'
Publication date: 01/01/2013
Field of study

This is the pre-print version of the final published paper that is available from the link belowSearches for anomalous top quark-antiquark production are presented, based on pp collisions at √s=8 TeV . The data, corresponding to an integrated luminosity of 19:7 fb^-1, were collected with the CMS detector at the LHC. The observed tt invariant mass spectrum is found to be compatible with the standard model prediction. Limits on the production cross section times branching fraction probe, for the first time, a region of parameter space for certain models of new physics not yet constrained by precision measurements

Repositorio Institucional de la Universidad de Oviedo

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