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Measurement of the forward $Z$ boson production cross-section in $pp$ collisions at $\sqrt{s}$ = 7 TeV (1505.07024v2)

Published 26 May 2015 in hep-ex

Abstract: A measurement of the production cross-section for $Z$ bosons that decay to muons is presented. The data were recorded by the LHCb detector during $pp$ collisions at a centre-of-mass energy of 7 TeV, and correspond to an integrated luminosity of 1.0 fb${-1}$. The cross-section is measured for muons in the pseudorapidity range $2.0 < \eta < 4.5$ with transverse momenta $p_{T} > 20$ GeV/c. The dimuon mass is restricted to $60 < M_{\mu{+}\mu{-}} < 120$ GeV/c${2}$. The measured cross-section is $$\sigma_{Z\rightarrow\mu{+}\mu{-}} = (76.0 \pm 0.3 \pm 0.5 \pm 1.0 \pm 1.3) \, \text{pb}$$ where the uncertainties are due to the sample size, systematic effects, the beam energy and the luminosity. This result is in good agreement with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics. The cross-section is also measured differentially as a function of kinematic variables of the $Z$ boson. Ratios of the production cross-sections of electroweak bosons are presented using updated LHCb measurements of $W$ boson production. A precise test of the Standard Model is provided by the measurement of the ratio $$\frac{\sigma_{W{+}\rightarrow\mu{+}\nu_{\mu}} + \sigma_{W{-}\rightarrow\mu{-}\bar{\nu}{\mu}}}{\sigma{Z\rightarrow\mu{+}\mu{-}}} = 20.63\pm0.09\pm0.12\pm0.05,$$ where the uncertainty due to luminosity cancels.

Citations (203)

Summary

Measurement of Forward ZZ Boson Production at 7 TeV in pppp Collisions

This paper presents a meticulous analysis of the forward production cross-section of ZZ bosons in proton-proton (pppp) collisions at a center-of-mass energy of 7 TeV. The data were collected using the LHCb detector at CERN, corresponding to an integrated luminosity of 1.0 fb1^{-1}. The ZZ bosons are identified through their decay into muon pairs, a clean channel highly favored due to its distinct signature and reduced background noise.

Highlights and Findings

  • Cross-section Measurement: The production cross-section for the Zμ+μZ \rightarrow \mu^+ \mu^- process is quantified at σZμ+μ=(76.0±0.3±0.5±1.0±1.3)\sigma_{Z\rightarrow\mu^{+}\mu^{-}} = (76.0 \pm 0.3 \pm 0.5 \pm 1.0 \pm 1.3) pb. The quoted uncertainties cover statistical, systematic, beam energy, and luminosity errors. This measurement aligns well with predictions from NNLO perturbative QCD calculations, confirming the robustness of the Standard Model (SM) under the experimental conditions.
  • Kinematic Range and Differential Cross-sections: Measurements focus on muons within the pseudorapidity range 2.0<η<4.52.0 < \eta < 4.5 and transverse momenta pT>20p_T > 20 GeV/c. The dimuon invariant mass is required to be within 60<Mμ+μ<12060 < M_{\mu^{+}\mu^{-}} < 120 GeV/c2^2. Additionally, differential cross-sections are reported as functions of the ZZ boson's rapidity (yZy_Z), transverse momentum (pT,Zp_{T,Z}), and ϕZ\phi^*_Z. These differential measurements provide valuable insights into parton distribution functions (PDFs) and the dynamics of electroweak interactions.
  • Electroweak Boson Ratios: The analysis extends to the ratio of WW to ZZ boson production cross-sections, delivering stringent tests for the consistency of SM predictions. The ratio (σW+μ+νμ+σWμνˉμσZμ+μ)\left( \frac{\sigma_{W^{+}\rightarrow\mu^{+}\nu_{\mu}} + \sigma_{W^{-}\rightarrow\mu^{-}\bar{\nu}_{\mu}}}{\sigma_{Z\rightarrow\mu^{+}\mu^{-}}} \right) is experimentally determined with a high degree of precision, RW/Z=20.63±0.09±0.12±0.05R_{W/Z} = 20.63 \pm 0.09 \pm 0.12 \pm 0.05.
  • Improved Precision: By revisiting the WW boson production analyses using enhanced trigger efficiency data, previously measured cross-section values for W+W^+ and WW^- bosons are updated, achieving significantly reduced uncertainties.

Implications and Future Developments

The results provide critical inputs for refining PDF models by testing their validity at non-central rapidities and expanding the constraints on fundamental parameters of the SM. The ongoing precision of such measurements will enhance the understanding of QCD interactions, particularly in the forward region, invaluable for future explorations at higher energies and luminosities, including those at the High-Luminosity LHC (HL-LHC).

Given these findings, subsequent research may delve into the subtleties of QCD corrections and potential beyond-the-Standard-Model effects observable at high-energy colliders. Moreover, the techniques developed and refined through this analysis could aid in the precision measurements of other processes involving electroweak bosons. The meticulous focus on systematic uncertainties, alongside statistical precision, sets a benchmark for similar measurements across experimental platforms.