Measurements of the associated production of a W boson and a charm quark in proton–proton collisions at s=8TeV\sqrt{s}=8\,\text {TeV}

Collaboration
Dec 1, 2021
52 pages
Published in:
  • Eur.Phys.J.C 82 (2022) 12, 1094
  • Published: Dec 5, 2022
e-Print:
Report number:
  • CMS-SMP-18-013,
  • CERN-EP-2021-206
Experiments:

Citations per year

20212022202320242025024681012
Abstract: (Springer)
Measurements of the associated production of a W boson and a charm (c{\text {c}}) quark in proton–proton collisions at a centre-of-mass energy of 8TeV\,\text {TeV} are reported. The analysis uses a data sample corresponding to a total integrated luminosity of 19.7fb1\,\text {fb}^{-1} collected by the CMS detector at the LHC. The W bosons are identified through their leptonic decays to an electron or a muon, and a neutrino. Charm quark jets are selected using distinctive signatures of charm hadron decays. The product of the cross section and branching fraction \sigma (\text {p}\text {p}\rightarrow \text {W}+ {\text {c}}+ \text {X}) {\mathcal {B}}(\text {W}\rightarrow \ell \upnu ), where =e\ell = \text {e} or \upmu , and the cross section ratio σ(ppW++cˉ+X)/σ(ppW+c+X)\sigma (\text {p}\text {p}\rightarrow {{\text {W}}^{+} + \bar{{\text {c}}} + \text {X}}) / \sigma (\text {p}\text {p}\rightarrow {{\text {W}}^{-} + {\text {c}}+ \text {X}}) are measured in a fiducial volume and differentially as functions of the pseudorapidity and of the transverse momentum of the lepton from the W boson decay. The results are compared with theoretical predictions. The impact of these measurements on the determination of the strange quark distribution is assessed.
Note:
  • p p: colliding beams
  • W: associated production
  • charm: associated production
  • p p: scattering
  • lepton: transverse momentum
  • quark: jet
  • jet: charm
  • charm: particle identification
  • W: leptonic decay
  • cross section: ratio: measured