Abstract

The production of W± bosons is studied in proton-lead (pPb) collisions at a nucleon-nucleon centre-of-mass energy of sNN=8.16TeV. Measurements are performed in the W±→μ±νμ channel using a data sample corresponding to an integrated luminosity of 173.4±6.1nb−1, collected by the CMS Collaboration at the LHC. The number of positively and negatively charged W bosons is determined separately in the muon pseudorapidity region in the laboratory frame |ηlabμ|<2.4 and transverse momentum pTμ>25GeV/c. The W± boson differential cross sections, muon charge asymmetry, and the ratios of W± boson yields for the proton-going over the Pb-going beam directions are reported as a function of the muon pseudorapidity in the nucleon-nucleon centre-of-mass frame. The measurements are compared to the predictions from theoretical calculations based on parton distribution functions (PDFs) at next-to-leading-order. The results favour PDF calculations that include nuclear modifications and provide constraints on the nuclear PDF global fits.

Highlights

  • The production of electroweak (EW) gauge bosons is considered to be a powerful probe of the parton distribution functions (PDFs) of the proton [1]

  • The nuclear PDFs are expected to be enhanced for partons carrying a momentum fraction in the range 5 × 10−2 x 10−1 in the so-called antishadowing region, and suppressed for x 10−2 in the shadowing region [9], with the modifications depending on the scale Q 2

  • The measurements are compared to theoretical predictions from both proton parton distribution functions (PDFs) (CT14) and nuclear PDF (CT14+EPPS16, CT14+nCTEQ15) sets

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Summary

Introduction

The production of electroweak (EW) gauge bosons is considered to be a powerful probe of the parton distribution functions (PDFs) of the proton [1]. The measurements of EW boson production in proton-nucleus and nucleus-nucleus collisions, available for the first time at centreof-mass energies of the TeV scale, provide constraints on nuclear modifications of the PDFs [5,6,7,8]. The nuclear PDFs (nPDFs) are expected to be enhanced for partons carrying a momentum fraction in the range 5 × 10−2 x 10−1 in the so-called antishadowing region, and suppressed for x 10−2 in the shadowing region [9], with the modifications depending on the scale Q 2. Because of the limited amount and type of experimental data sets available for nuclear collisions, the determination of the nuclear parton densities is less precise than for the free-proton case. The nPDF uncertainties are one of the main limitations of the precision of quantum chromodynamics (QCD) calculations describing hardscattering processes in nuclear collisions at high energies [7]

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