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|a Sirunyan, A. M.
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|a Tumasyan, A.
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|a Adam, W.
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|a Ambrogi, F.
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|a Bergauer, T.
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|a Dragicevic, M.
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|a Erö, J.
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|a Escalante Del Valle, A.
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|a Frühwirth, R.
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|a Jeitler, M.
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|a Krammer, N.
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|a Lechner, L.
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|a Liko, D.
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|a Madlener, T.
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|a Mikulec, I.
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|a Pitters, F. M.
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|a Rad, N.
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|a Schieck, J.
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|a Study of Drell-Yan dimuon production in proton-lead collisions at s NN $$ \sqrt{s_{\mathrm{NN}}} $$ = 8.16 TeV
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|b Springer Berlin Heidelberg,
|c 2021-11-01T14:33:31Z.
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|z Get fulltext
|u https://hdl.handle.net/1721.1/136809
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|a Abstract Differential 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 8.16 TeV. 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 ϕ* are measured, where ϕ* 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.
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