Abstract
Abstract Weak bosons do not participate in the strong interaction, and thus constitute clean probes of the initial state of nucleus–nucleus collisions. The comparison of their production cross sections in pp and in nuclear collisions provides constraints on the nuclear parton distribution functions. Despite the low production cross section of weak bosons, compared to other nuclear processes, the relatively clean signal of their leptonic decay channels allows their detection and reconstruction. A first analysis of PbPb data has confirmed the medium-blind characteristic of the electroweak bosons. This paper reports measurements of Z and W bosons, produced in PbPb and pp collisions at nucleon–nucleon centre of mass energy s NN = 2.76 TeV with the CMS detector. The Z boson yield and the nuclear modification factor ( R AA ) corresponding to an integrated luminosity of 150 μb − 1 are presented, as a function of the centrality, of the Z rapidity and p T , both in the muonic and electronic channels. Event centrality and muon pseudorapidity dependencies of the W production yields are presented separately for W + and W − .
Highlights
The unprecedented high energies and luminosities reached in heavy-ion collisions at the LHC have opened the possibility of producing significant yields of the weakly interacting bosons, Z and W
Weak boson do not participate in the strong interaction, and constitute clean probes of the initial state of nucleus-nucleus collisions
These bosons are produced in the primary binary nucleon-nucleon collisions and decay before the quark-gluon plasma expected formation time [1]. Their leptonic decay products do not interact with the hot and dense coloured matter. They are only sensitive to the initial state of the collision and in particular to the parton distribution functions (PDF) in the nuclei
Summary
The unprecedented high energies and luminosities reached in heavy-ion collisions at the LHC have opened the possibility of producing significant yields of the weakly interacting bosons, Z and W. These bosons are produced in the primary binary nucleon-nucleon collisions and decay before the quark-gluon plasma expected formation time [1]. Their leptonic decay products do not interact with the hot and dense coloured matter. They are only sensitive to the initial state of the collision and in particular to the parton distribution functions (PDF) in the nuclei
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