The first measurement of the Z boson production cross-section at centre-of-mass energy √s=5.02TeV in the forward region is reported, using pp collision data collected by the LHCb experiment in year 2017, corresponding to an integrated luminosity of 100±2pb−1. The production cross-section is measured for final-state muons in the pseudorapidity range 2.0<η<4.5 with transverse momentum pT>20GeV/c. The integrated cross-section is determined to be \[ \sigma_{Z \rightarrow \mu^{+}\mu^{-}} = 39.6 \pm 0.7 (\rm{stat}) \pm 0.6 (\rm{syst}) \pm 0.8 (\rm{lumi}) \rm{pb} \] for the di-muon invariant mass in the range 60<Mμμ<120GeV/c2. This result and the differential cross-section results are in good agreement with theoretical predictions at next-to-next-to-leading order in the strong coupling. Based on a previous LHCb measurement of the Z boson production cross-section in pPb collisions at √sNN=5.02 TeV, the nuclear modification factor RpPb is measured for the first time at this energy. The measured values are 1.2+0.5−0.3(stat)±0.1(syst) in the forward region (1.53<y∗μ<4.03) and 3.6+1.6−0.9(stat)±0.2(syst) in the backward region (−4.97<y∗μ<−2.47), where y∗μ represents the muon rapidity in the centre-of-mass frame.
Mass distribution of the Z→μ+μ− signal candidates. The data are overlaid with model of the signal and background models. The signal component is scaled such that the sum of the signal and background matches the integral of the data. |
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Final state radiation correction estimated for the (top-left) yZ , (top-right) pZT , and (bottom) ϕ∗η differential cross-section measurements. The error bars represent the total (statistical and systematic) uncertainties. |
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(Left) Measured single differential cross-section as a function of yZ , pZT and ϕ∗η compared with different theoretical predictions. (Right) Ratio of theoretical predictions to measured values, with the horizontal bars showing the uncertainty from the PDFs. The green band, centered at unity, shows the uncertainty of the measurement. |
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Comparison of the integrated cross-section, σZ→μ+μ−, between data and theoretical predictions. The bands correspond to the data, with the inner band corresponding to the statistical uncertainty and the outer bands corresponding to the systematic uncertainty and total uncertainty. |
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Measured σZ→μ+μ− for pp collisions, as a function of √s. The uncertainty on the data is smaller than the marker size. The data are overlaid with a curve showing the theoretical prediction. |
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Invariant mass distributions of heavy-flavour samples with (left) PV fit quality χ2>95 and (right) Iμ<91% applied to both muons. Only statistical uncertainties are shown. |
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Muon tracking, identification and trigger efficiency as a function of pseudorapidity, estimated from the data and simulation at 5.02 Te V and 13 Te V . |
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Statistical correlation matrices for the differential cross-section measurements as functions of (top-left) yZ , (top-right) pZT and (bottom) ϕ∗η . |
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Correlation matrices for the efficiency uncertainties as functions of (top-left) yZ , (top-right) pZT and (bottom) ϕ∗η . |
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Animated gif made out of all figures. |
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Summary of the background composition in the Z→μ+μ− data sample of candidates satisfying the signal selection. |
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The uncertainties for the integrated Z→μ+μ− cross-section measurement. |
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Final state radiation correction used in the yZ cross-section measurement. The first uncertainty is statistical and the second is systematic. |
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Final state radiation correction used in the pZT cross-section measurement. The first uncertainty is statistical and the second is systematic. |
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Final state radiation correction used in the ϕ∗η cross-section measurement. The first uncertainty is statistical and the second is systematic. |
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The muon tracking, muon identification and trigger efficiency in each pseudorapidity bin. |
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Systematic uncertainties on the single differential cross-sections in bins of yZ , presented in percentage. |
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Systematic uncertainties on the single differential cross-sections in bins of pZT , presented in percentage. |
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Systematic uncertainties on the single differential cross-sections in bins of ϕ∗η , presented in percentage. |
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Measured single differential cross-sections in bins of yZ . The first uncertainty is statistical, the second systematic, and the third is from the uncertainty on the integrated luminosity. |
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Measured single differential cross-sections in bins of pZT . The first uncertainty is statistical, the second systematic, and the third is due to the luminosity. |
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Measured single differential cross-sections in bins of ϕ∗η . The first uncertainty is statistical, the second systematic, and the third is due to the luminosity. |
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Statistical correlation matrix for the one-dimensional yZ measurement. |
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Statistical correlation matrix for the one-dimensional pZT measurement. |
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Statistical correlation matrix for the one-dimensional ϕ∗η measurement. |
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Correlation matrix for the efficiency uncertainty of the one-dimensional yZ measurement. |
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Correlation matrix for the efficiency uncertainty of the one-dimensional pZT measurement. |
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Correlation matrix for the efficiency uncertainty of the one-dimensional ϕ∗η measurement. |
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Created on 29 March 2025.