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.
Highlights
A measurement of the production cross-section for Z bosons that decay to muons is presented
Cross-sections are quoted in the kinematic range defined by the measurement and are corrected for quantum electrodynamic (QED) final-state radiation (FSR) in order to provide a consistent comparison with next-toleading order (NLO) and NNLO QCD predictions
The measured rapidity distribution as shown in figure 2 is compared to the prediction from Fewz [30, 31] with six different PDF sets
Summary
The LHCb detector [14, 15] is a single-arm forward spectrometer covering the pseudorapidity range 2 < η < 5, designed for the study of particles containing b or c quarks. The absolute luminosity scale was measured during dedicated data taking periods, using both Van der Meer scans [21] and beam-gas imaging methods [22]. Both methods give similar results, which are combined to give the final luminosity estimate with an uncertainty of 1.7% [23]. This analysis uses the same data set as in ref. Total uncertainties correspond to the PDF and αs uncertainties at 68.3% confidence level and scale uncertainties, added in quadrature
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