Measurement of the Upsilon(1s), Upsilon(2s), and Upsilon(3s) Cross Sections in Pp Collisions at Root S=7 Tev

dc.contributor.author Karapınar, Güler
dc.coverage.doi 10.1016/j.physletb.2013.10.033 en_US
dc.date.accessioned 2021-01-24T18:47:22Z
dc.date.available 2021-01-24T18:47:22Z
dc.date.issued 2013
dc.description.abstract The Upsilon(1S), Upsilon(2S), and Upsilon(3S) production cross sections are measured using a data sample corresponding to an integrated luminosity of 35.8 +/- 1.4 pb(-1) of proton-proton collisions at root s = 7 TeV, collected with the CMS detector at the LHC. The Upsilon resonances are identified through their decays to dimuons. Integrated over the Upsilon transverse momentum range p(T)(Upsilon) < 50 GeV/c and rapidity range vertical bar y(Upsilon)vertical bar < 2.4, and assuming unpolarized Upsilon production, the products of the Upsilon production cross sections and dimuon branching fractions are sigma (pp -> Upsilon(1S)X) . B(Upsilon(1S) -> mu(+)mu(-)) = (8.55 +/- 0.05(-0.50)(+0.56) +/- 0.34) nb, sigma (pp -> Upsilon(2S)X) . B(Upsilon(2S) -> mu(+)mu(-)) = (2.21 +/- 0.03(-0.14)(+0.16) +/- 0.09) nb, sigma (pp -> Upsilon(3S)X) . B(Upsilon(3S) -> mu(+)mu(-)) = (1.11 +/- 0.02(-0.08)(+0.10) +/- 0.04) nb, where the first uncertainty is statistical, the second is systematic, and the third is from the uncertainty in the integrated luminosity. The differential cross sections in bins of transverse momentum and rapidity, and the cross section ratios are presented. Cross section measurements performed within a restricted muon kinematic range and not corrected for acceptance are also provided. These latter measurements are independent of Upsilon polarization assumptions. The results are compared to theoretical predictions and previous measurements. (C) 2013 CERN. Published by Elsevier B.V. All rights reserved. en_US
dc.description.sponsorship We congratulate our colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS effort. In addition, we gratefully acknowledge the computing centres and personnel of the Worldwide LHC Computing Grid for delivering so effectively the computing infrastructure essential to our analyses. Finally, we acknowledge the enduring support for the construction and operation of the LHC and the CMS detector provided by the following funding agencies: BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MEYS (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 (Republic of 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); ThEPCenter, IPST and NSTDA (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA). Individuals have received support from the Marie-Curie programme and the European Research Council and EPLANET (European Union); the Leventis Foundation; the A.P. Sloan Foundation; the Alexander von Humboldt Foundation; the Belgian Federal Science Policy Office; the Fonds pour la Formation a la Recherche dans l'Industrie et dans l'Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); 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 programme of Foundation for Polish Science, cofinanced from European Union, Regional Development Fund. en_US
dc.identifier.doi 10.1016/j.physletb.2013.10.033 en_US
dc.identifier.issn 0370-2693
dc.identifier.uri https://doi.org/10.1016/j.physletb.2013.10.033
dc.identifier.uri https://hdl.handle.net/11147/10649
dc.language.iso en en_US
dc.publisher Elsevier Ltd. en_US
dc.relation.ispartof Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics en_US
dc.rights info:eu-repo/semantics/openAccess en_US
dc.subject CMS en_US
dc.subject Physics en_US
dc.subject Quarkonia en_US
dc.subject Upsilon en_US
dc.subject Dimuons en_US
dc.title Measurement of the Upsilon(1s), Upsilon(2s), and Upsilon(3s) Cross Sections in Pp Collisions at Root S=7 Tev en_US
dc.type Article en_US
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gdc.description.department İzmir Institute of Technology. Rectorate en_US
gdc.description.endpage 125 en_US
gdc.description.issue 01.Mar en_US
gdc.description.publicationcategory Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı en_US
gdc.description.scopusquality Q1
gdc.description.startpage 101 en_US
gdc.description.volume 727 en_US
gdc.description.wosquality Q1
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gdc.oaire.keywords CMS; physics; Quarkonia; Upsilon; Dimuons
gdc.oaire.keywords PARTICLE PHYSICS; LARGE HADRON COLLIDER; CMS
gdc.oaire.keywords High Energy Physics - Experiment
gdc.oaire.keywords High Energy Physics - Experiment (hep-ex)
gdc.oaire.keywords UNIVERSAL MONTE-CARLO
gdc.oaire.keywords [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]
gdc.oaire.keywords Upsilon
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gdc.oaire.keywords QC Physics / fizika
gdc.oaire.keywords Physique des particules élémentaires
gdc.oaire.keywords LHC; CMS; HEP
gdc.oaire.keywords PARTICLE PHYSICS
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