A precision measurement of the $Z$ boson production cross-section at $\sqrt{s} = 13$ TeV in the forward region is presented, using $pp$ collision data collected by the LHCb detector, corresponding to an integrated luminosity of 5.1 fb$^{-1}$. The production cross-section is measured using $Z\rightarrow\mu^+\mu^-$ events within the fiducial region defined as pseudorapidity $2.0<\eta<4.5$ and transverse momentum $p_{T}>20$ GeV/$c$ for both muons and dimuon invariant mass $60<M_{\mu\mu}<120$ GeV/$c^2$. The integrated cross-section is determined to be \begin{equation*} \sigma(Z\rightarrow\mu^+\mu^-) = 196.4 \pm 0.2 \pm 1.6 \pm 3.9 pb, \end{equation*} where the first uncertainty is statistical, the second is systematic, and the third is due to the luminosity determination. The measured results are in agreement with theoretical predictions within uncertainties.
Comparison of the invariant mass distribution between data and the sum of signal and background contributions for the selected $ Z \rightarrow \mu ^+\mu ^- $ candidates. |
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Final state radiation correction estimated for the (top-left) $ y^{\mathrm{Z}}$ , (top-right) $ p_{\mathrm{T}}^{Z}$ , and (bottom) $\phi_{\eta}^{*}$ differential cross-section measurements. The error bars represent the total (statistical and systematic) uncertainties. |
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(Top) Measured single differential cross-section in regions of $ y^{\mathrm{Z}}$ , compared with different theoretical predictions. In order to present the measurements more clearly, data bands are drawn wider than the width of the interval. (Bottom) Ratio of theoretical predictions to measured values, with the horizontal bars showing the uncertainty from the PDFs. |
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(Top) Measured single differential cross-section in regions of $ p_{\mathrm{T}}^{Z}$ , compared with different theoretical predictions. (Bottom) Ratio of ResBos predictions to measurement, with the horizontal bars showing the uncertainty from the PDFs. |
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(Top) Measured single differential cross-section in regions of $\phi_{\eta}^{*}$ , compared with different theoretical predictions. (Bottom) Ratio of ResBos predictions to measurement, with the horizontal bars showing the uncertainty from the PDFs. |
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Measured double differential cross-section as a function of $ p_{\mathrm{T}}^{Z}$ in regions of $ y^{\mathrm{Z}}$ , compared with ResBos predictions, with the horizontal bars showing the uncertainty from the PDFs. |
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Ratios of ResBos predictions to measurements as a function of $ p_{\mathrm{T}}^{Z}$ in regions of $ y^{\mathrm{Z}}$ , with the horizontal bars showing the uncertainty from the PDFs. |
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Measured double differential cross-section as a function of $\phi_{\eta}^{*}$ in regions of $ y^{\mathrm{Z}}$ , compared with ResBos predictions, with the horizontal bars showing the uncertainty from the PDFs. |
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Ratios of ResBos predictions to measurements as a function of $\phi_{\eta}^{*}$ in regions of $ y^{\mathrm{Z}}$ , with the horizontal bars showing the uncertainty from the PDFs. |
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Comparison of the integrated cross-section, $\sigma_{ Z \rightarrow \mu ^+\mu ^- }$, 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. The open circles correspond to the different theoretical predictions. The diamond point corresponds to the previous LHCb measurement \cite{LHCb-PAPER-2016-021}. |
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Final state radiation correction estimated for double differential cross section measurement for (left) $ y^{\mathrm{Z}} - p_{\mathrm{T}}^{Z} $ measurement, and for (right) $ y^{\mathrm{Z}} -\phi_{\eta}^{*} $ measurement. |
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Statistical correlation matrix of the cross-section measurements in one-dimensional interval regions of (top-left) $ y^{\mathrm{Z}}$ , (top-right) $ p_{\mathrm{T}}^{Z}$ and (bottom) $\phi_{\eta}^{*}$ . More details about the `interval number' can be found from Table ??? and Table ???. |
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Statistical correlation matrix of the cross-section measurements in two-dimensional interval regions of (left) $ y^{\mathrm{Z}} - p_{\mathrm{T}}^{Z} $ and (right) $ y^{\mathrm{Z}} -\phi_{\eta}^{*} $. More details about the `interval number' can be found in Table ??? and Table ???. |
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Correlation matrix of efficiencies uncertainty for one-dimensional (top-left) $ y^{\mathrm{Z}}$ , (top-right) $ p_{\mathrm{T}}^{Z}$ and (bottom) $\phi_{\eta}^{*}$ measurements. More details about the `interval number' can be found in Table ??? and Table ???. |
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Correlation matrix of efficiencies uncertainty for two-dimensional (left) $ y^{\mathrm{Z}} - p_{\mathrm{T}}^{Z} $ and (right) $ y^{\mathrm{Z}} -\phi_{\eta}^{*} $ measurements. More details about the `interval number' can be found in Table ??? and Table ???. |
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Animated gif made out of all figures. |
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Relative uncertainty for the integrated $ Z \rightarrow \mu ^+\mu ^- $ cross-section measurement. The total uncertainty is the quadratic sum of uncertainties from statistical, systematic and luminosity contributions. |
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Final state radiation correction used in the $ y^{\mathrm{Z}}$ cross-section measurement. The first uncertainty is statistical and the second is systematic. |
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Final state radiation correction used in the $ p_{\mathrm{T}}^{Z}$ cross-section measurement. The first uncertainty is statistical and the second is systematic. |
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Final state radiation correction used in the $\phi_{\eta}^{*}$ cross-section measurement. The first uncertainty is statistical and the second is systematic. |
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Correlation matrix of statistical uncertainty for one-dimensional $ y^{\mathrm{Z}}$ measurement. |
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Correlation matrix of statistical uncertainty for one-dimensional $ p_{\mathrm{T}}^{Z}$ measurement. |
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Correlation matrix of statistical uncertainty for one-dimensional $\phi_{\eta}^{*}$ measurement. |
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Correlation matrix of efficiency uncertainty for one-dimensional $ y^{\mathrm{Z}}$ measurement. |
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Correlation matrix of efficiency uncertainty for one-dimensional $ p_{\mathrm{T}}^{Z}$ measurement. |
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Correlation matrix of efficiency uncertainty for one-dimensional $\phi_{\eta}^{*}$ measurement. |
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Measured total $ Z $ -boson cross-section for different datasets. 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 interval regions of $ y^{\mathrm{Z}}$ . 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 interval regions of $ p_{\mathrm{T}}^{Z}$ . The first uncertainty is statistical, the second systematic, and the third is due to the luminosity. |
Table_13.pdf [67 KiB] HiDef png [99 KiB] Thumbnail [60 KiB] tex code |
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Measured single differential cross-sections in interval regions of $\phi_{\eta}^{*}$ . The first uncertainty is statistical, the second systematic, and the third is due to the luminosity. |
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Systematic uncertainties in the single differential cross-sections in interval regions of $ y^{\mathrm{Z}}$ , presented in percentage. The contributions from efficiency (Eff), background (BKG), final state radiation (FSR), closure test (Closure), and alignment and calibration (Alignment) are shown. |
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Systematic uncertainties in the single differential cross-sections in interval regions of $ p_{\mathrm{T}}^{Z}$ , presented in percentage. The contributions from efficiency (Eff), background (BKG), final state radiation (FSR), closure test (Closure), unfolding (Unfold), and alignment and calibration (Alignment) are shown. |
Table_16.pdf [62 KiB] HiDef png [129 KiB] Thumbnail [62 KiB] tex code |
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Systematic uncertainties in the single differential cross-sections in interval regions of $\phi_{\eta}^{*}$ , presented in percentage. The contributions from efficiency (Eff), background (BKG), final state radiation (FSR), closure test (Closure), and alignment and calibration (Alignment) are shown. |
Table_17.pdf [61 KiB] HiDef png [145 KiB] Thumbnail [71 KiB] tex code |
Created on 27 April 2024.