Please use this identifier to cite or link to this item: http://archive.cmb.ac.lk:8080/xmlui/handle/70130/6178
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dc.contributor.authorJayananda, M.K.-
dc.contributor.authorSonnadara, D.U.J.-
dc.contributor.authorWickramaratne, D.D.C.-
dc.date.accessioned2021-10-01T10:30:51Z-
dc.date.available2021-10-01T10:30:51Z-
dc.date.issued2021-
dc.identifier.citationThe CMS collaboration., Sirunyan, A.M., Tumasyan, A. et al. Study of Drell-Yan dimuon production in proton-lead collisions at sNN−−−√ = 8.16 TeV. J. High Energ. Phys. 2021, 182 (2021). https://doi.org/10.1007/JHEP05(2021)182en_US
dc.identifier.urihttps://doi.org/10.1007/JHEP05(2021)182-
dc.identifier.urihttp://archive.cmb.ac.lk:8080/xmlui/handle/70130/6178-
dc.description.abstractDifferential cross sections for the Drell-Yan process, including Z boson production, using the dimuon decay channel are measured in proton-lead (pPb) collisions at a nucleon-nucleon centre-of-mass energy of 8.16TeV. A data sample recorded with the CMS detector at the LHC is used, corresponding to an integrated luminosity of 173 nb−1. The differential cross section as a function of the dimuon mass is measured in the range 15– 600 GeV, for the first time in proton-nucleus collisions. It is also reported as a function of dimuon rapidity over the mass ranges 15–60 GeV and 60–120 GeV, and ratios for the p-going over the Pb-going beam directions are built. In both mass ranges, the differential cross sections as functions of the dimuon transverse momentum pT and of a geometric variable are measured, where highly correlates with pT but is determined with higher precision. In the Z mass region, the rapidity dependence of the data indicate a modification of the distribution of partons within a lead nucleus as compared to the proton case. The data are more precise than predictions based upon current models of parton distributions.en_US
dc.language.isoenen_US
dc.subjectHadron-Hadron scattering (experiments), Relativistic heavy ion physicsen_US
dc.titleStudy of Drell-Yan dimuon production in proton-lead collisions at sNN−−−√ = 8.16 TeVen_US
dc.typeArticleen_US
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