Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/2298
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dc.contributor.authorCMS Collaborationen_US
dc.contributor.authorKhachatryan, V.en_US
dc.contributor.authorSHARMA, SEEMA et al.en_US
dc.date.accessioned2019-03-15T11:27:04Z
dc.date.available2019-03-15T11:27:04Z
dc.date.issued2015-10en_US
dc.identifier.citationPhysics Letters B, 749, 14-34.en_US
dc.identifier.issn0370-2693en_US
dc.identifier.issn1873-2445en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/2298-
dc.identifier.urihttps://doi.org/10.1016/j.physletb.2015.07.037en_US
dc.description.abstractDifferential cross sections as a function of transverse momentum pT are presented for the production of ϒ(nS) (n = 1, 2, 3) states decaying into a pair of muons. Data corresponding to an integrated luminosity of 4.9fb−1 in pp collisions at s=7TeV were collected with the CMS detector at the LHC. The analysis selects events with dimuon rapidity |y|<1.2 and dimuon transverse momentum in the range 10<pT<100GeV. The measurements show a transition from an exponential to a power-law behavior at pT≈20GeV for the three ϒ states. Above that transition, the ϒ(3S) spectrum is significantly harder than that of the ϒ(1S). The ratios of the ϒ(3S) and ϒ(2S) differential cross sections to the ϒ(1S) cross section show a rise as pT increases at low pT, then become flatter at higher pTen_US
dc.language.isoenen_US
dc.publisherElsevier B.V.en_US
dc.subjectCMSen_US
dc.subjectUpsilonen_US
dc.subjectB-Physicsen_US
dc.subjectCross sectionen_US
dc.subjectQuantum chromodynamicsen_US
dc.subjectYield determination procedureen_US
dc.subject2015en_US
dc.titleMeasurements of the Upsilon(1S), Upsilon(2S), and Upsilon(3S) differential cross sections in pp collisions at root s=7 TeVen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysics Letters Ben_US
dc.publication.originofpublisherForeignen_US
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