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dc.contributor.authorTumasyan, Armenpt_BR
dc.contributor.authorSilveira, Gustavo Gil dapt_BR
dc.contributor.authorCMS Collaborationpt_BR
dc.date.accessioned2023-05-10T03:26:54Zpt_BR
dc.date.issued2022pt_BR
dc.identifier.issn0370-2693pt_BR
dc.identifier.urihttp://hdl.handle.net/10183/257851pt_BR
dc.description.abstractProduction cross sections of Υ(1S), Υ(2S), and Υ(3S) states decaying into μ+μ− in proton-lead (pPb) collisions are reported using data collected by the CMS experiment at √sNN = 5.02 TeV. A comparison is made with corresponding cross sections obtained with pp data measured at the same collision energy and scaled by the Pb nucleus mass number. The nuclear modification factor for Υ(1S) is found to be RpPb(Υ(1S)) = 0.806 ±0.024 (stat) ±0.059 (syst). Similar results for the excited states indicate a sequential suppression pattern, such that RpPb(Υ(1S)) > RpPb(Υ(2S)) > RpPb(Υ(3S)). The suppression of all states is much less pronounced in pPb than in PbPb collisions, and independent of transverse momentum pΥ T and center-of-mass rapidity yΥ CM of the individual Υ state in the studied range pΥ T < 30 GeV/c and |yΥ CM| < 1.93. Models that incorporate final-state effects of bottomonia in pPb collisions are in better agreement with the data than those which only assume initial-state modifications.en
dc.format.mimetypeapplication/pdfpt_BR
dc.language.isoengpt_BR
dc.relation.ispartofPhysics letters. B. Amsterdam. Vol. 835 (Dec. 2022), 137397, 28 p.pt_BR
dc.rightsOpen Accessen
dc.subjectCMSen
dc.subjectAceleradores de partículaspt_BR
dc.subjectBottomoniumen
dc.subjectColisao de ions pesadospt_BR
dc.subjectQuarkonium suppressionen
dc.subjectMésons Ypt_BR
dc.subjectQuark gluon plasmaen
dc.subjectHeavy ion collisionsen
dc.titleNuclear modification of Y states in pPb collisions at √snn = 5.02 TeVpt_BR
dc.typeArtigo de periódicopt_BR
dc.identifier.nrb001164039pt_BR
dc.type.originEstrangeiropt_BR


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