CMS logoCMS event Hgg
Compact Muon Solenoid
LHC, CERN

CMS-SMP-24-005 ; CERN-EP-2024-293
Measurement of the inclusive WZ production cross section in pp collisions at $ \sqrt{s}= $ 13.6 TeV
Submitted to J. High Energy Phys.
Abstract: The inclusive WZ production cross section is measured in proton-proton collisions at a centre-of-mass energy of 13.6 TeV, using data collected during 2022 with the CMS detector, corresponding to an integrated luminosity of 34.7 fb$ ^{-1} $. The measurement uses multileptonic final states and a simultaneous likelihood fit to the number of events in four different lepton flavour categories: $ \mathrm{e}\mathrm{e}\mathrm{e} $, $ \mathrm{e}\mathrm{e}\mu $, $ \mu\mu\mathrm{e} $, and $ \mu\mu\mu $. The selection is optimized to minimize the number of background events, and relies on an efficient prompt lepton discrimination strategy. The WZ production cross section is measured in a phase space defined within a 30 GeV window around the Z boson mass, as $ \sigma_{\text{total}}(\mathrm{p}\mathrm{p}\to\mathrm{W}\mathrm{Z})= $ 55.2 $ \pm $ 1.2 (stat) $ \pm $ 1.2 (syst) $ \pm $ 0.8 (lumi) $ \pm $ 0.1 (theo) pb. In addition, the cross section is measured in a fiducial phase space closer to the detector-level requirements. All the measurements presented in this paper are in agreement with standard model predictions.
Figures & Tables Summary References CMS Publications
Figures

png pdf
Figure 1:
Leading-order Feynman diagrams for WZ production in pp collisions from the $ s $ channel (left), $ t $ channel (centre), and $ u $ channel (right).

png pdf
Figure 1-a:
Leading-order Feynman diagrams for WZ production in pp collisions from the $ s $ channel (left), $ t $ channel (centre), and $ u $ channel (right).

png pdf
Figure 1-b:
Leading-order Feynman diagrams for WZ production in pp collisions from the $ s $ channel (left), $ t $ channel (centre), and $ u $ channel (right).

png pdf
Figure 1-c:
Leading-order Feynman diagrams for WZ production in pp collisions from the $ s $ channel (left), $ t $ channel (centre), and $ u $ channel (right).

png pdf
Figure 2:
Distribution of observables in the ZZ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $3. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 2-a:
Distribution of observables in the ZZ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $3. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 2-b:
Distribution of observables in the ZZ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $3. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 2-c:
Distribution of observables in the ZZ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $3. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 2-d:
Distribution of observables in the ZZ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $3. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 3:
Distribution of the invariant mass of $ \ell $Z1 and $ \ell $Z2 in the ZZ CR accounting for the fit to data. The left (right) distribution shows the case in which the leptons are electrons (muons). The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 3-a:
Distribution of the invariant mass of $ \ell $Z1 and $ \ell $Z2 in the ZZ CR accounting for the fit to data. The left (right) distribution shows the case in which the leptons are electrons (muons). The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 3-b:
Distribution of the invariant mass of $ \ell $Z1 and $ \ell $Z2 in the ZZ CR accounting for the fit to data. The left (right) distribution shows the case in which the leptons are electrons (muons). The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 4:
Distribution of observables in the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 4-a:
Distribution of observables in the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 4-b:
Distribution of observables in the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 4-c:
Distribution of observables in the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 4-d:
Distribution of observables in the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 5:
Distribution of observables in the $ \mathrm{X}\gamma $ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 5-a:
Distribution of observables in the $ \mathrm{X}\gamma $ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 5-b:
Distribution of observables in the $ \mathrm{X}\gamma $ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 5-c:
Distribution of observables in the $ \mathrm{X}\gamma $ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 5-d:
Distribution of observables in the $ \mathrm{X}\gamma $ CR accounting for the fit to data, described in Section 8. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched bands show the total uncertainty in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 6:
Distributions of several observables in the SR accounting for the fit to data. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched band includes all systematic uncertainties in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 6-a:
Distributions of several observables in the SR accounting for the fit to data. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched band includes all systematic uncertainties in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 6-b:
Distributions of several observables in the SR accounting for the fit to data. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched band includes all systematic uncertainties in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 6-c:
Distributions of several observables in the SR accounting for the fit to data. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched band includes all systematic uncertainties in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 6-d:
Distributions of several observables in the SR accounting for the fit to data. Clockwise from upper left to lower right: flavour composition, $ p_{\mathrm{T}} $ of $ \ell $Z1, $ p_{\mathrm{T}} $ of $ \ell $Z2, and $ p_{\mathrm{T}} $ of $ \ell $W. The hatched band includes all systematic uncertainties in the MC prediction. The vertical bars of the data account for the statistical uncertainty. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 7:
Distributions of several observables in the SR accounting for the fit to data. Clockwise from upper left to lower right: sum of charge of the final-state leptons, missing transverse momentum, invariant mass of the two leptons assigned to the Z boson decay, and that of the trilepton system. The hatched band includes all systematic uncertainties. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 7-a:
Distributions of several observables in the SR accounting for the fit to data. Clockwise from upper left to lower right: sum of charge of the final-state leptons, missing transverse momentum, invariant mass of the two leptons assigned to the Z boson decay, and that of the trilepton system. The hatched band includes all systematic uncertainties. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 7-b:
Distributions of several observables in the SR accounting for the fit to data. Clockwise from upper left to lower right: sum of charge of the final-state leptons, missing transverse momentum, invariant mass of the two leptons assigned to the Z boson decay, and that of the trilepton system. The hatched band includes all systematic uncertainties. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 7-c:
Distributions of several observables in the SR accounting for the fit to data. Clockwise from upper left to lower right: sum of charge of the final-state leptons, missing transverse momentum, invariant mass of the two leptons assigned to the Z boson decay, and that of the trilepton system. The hatched band includes all systematic uncertainties. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 7-d:
Distributions of several observables in the SR accounting for the fit to data. Clockwise from upper left to lower right: sum of charge of the final-state leptons, missing transverse momentum, invariant mass of the two leptons assigned to the Z boson decay, and that of the trilepton system. The hatched band includes all systematic uncertainties. When present, overflow events are included in the last bin of the observables. The ratio panels show the ratio between data (black markers) with respect to the total prediction after the fit to data. Processes with a small contribution to this region are grouped in the ``Other'' category.

png pdf
Figure 8:
Total WZ production cross section for each of the flavour-exclusive and for the flavour-inclusive categories. The vertical bands show different theoretical predictions for the WZ cross section at NLO in QCD (red dashed line) and NNLO QCD $\times$ NLO EW (blue solid line), as well as their corresponding scale uncertainties. For each measurement, the best fit value is denoted with a purple point, with two delimiters on the error bars that account for the statistical and total uncertainties.

png pdf
Figure 9:
Measurement obtained in this analysis (red filled marker) together with other WZ production cross section measurements at different centre-of-mass energies by the CMS [6,1,7] Collaboration, compared to the NNLO QCD $\times$ NLO EW predictions, as well as the pure NLO prediction, computed in all cases with MATRIX.
Tables

png pdf
Table 1:
Requirements for the definition of the signal and control regions of the analysis. Objects in parentheses relate to the ZZ CR.

png pdf
Table 2:
Summary of the input relative uncertainties. Numbers are presented in percentages over the total yields of the associated process on which they have an effect. All uncertainties are treated as shape variations on the templates used for the fit, with the exception of the normalization uncertainties in the backgrounds that are treated as flat variations of the corresponding yield.

png pdf
Table 3:
Definition of the fiducial and total regions. The lepton related quantities refer to ``dressed'' leptons. A dash symbol is used in cases the selection is not considered for the corresponding phase space.

png pdf
Table 4:
Number of selected events and their total uncertianty (by flavour channel) for the relevant processes in the signal region of the analysis accounting for the fit to data. The ``Background'' yield is the sum of all processes that are not WZ signal, and ``Prediction'' is the sum of all the processes, including WZ.

png pdf
Table 5:
Measured fiducial cross sections and their corresponding uncertainties for the flavour-exclusive and flavour-inclusive categories. The predictions from both POWHEG at NLO in QCD and LO EW as well as several ones obtained from MATRIX (NLO QCD, NNLO QCD, NNLO QCD $\times$ NLO EW) are also included.

png pdf
Table 6:
Flavour-inclusive total cross section result. The predictions from both POWHEG at NLO in QCD and LO EW as well as several ones obtained from MATRIX (NLO QCD, NNLO QCD, NNLO QCD $\times$ NLO EW) are also included.

png pdf
Table 7:
Breakdown of different sources of systematic uncertainties and their relative impact in each channel, as well as in the inclusive measurement; as a percentage of the total uncertainty. The dash symbol indicates that the specific uncertainty does not apply.
Summary
The inclusive WZ production cross section is measured in proton-proton collisions at a centre-of-mass energy of 13.6 TeV, using data collected during 2022 with the CMS detector, corresponding to an integrated luminosity of 34.7 fb$ ^{-1} $. The production cross sections in the total and fiducial phase spaces are measured in the inclusive case as well as in four combinations of final state flavour composition. The cross sections are measured in a fiducial phase space as $ \sigma_{\text{fiducial}}(\mathrm{p}\mathrm{p}\to\mathrm{W}\mathrm{Z})= $ 297.6 $ \pm $ 6.4 (stat) $ \pm $ 6.4 (syst) $ \pm $ 4.2 (lumi) $ \pm $ 0.5 (theo) fb, and in a less restricted phase space as $ \sigma_{\text{total}}(\mathrm{p}\mathrm{p}\to\mathrm{W}\mathrm{Z})= $ 55.2 $ \pm $ 1.2 (stat) $ \pm $ 1.2 (syst) $ \pm $ 0.8 (lumi) $ \pm $ 0.1 (theo) pb. All these measurements are shown to be in good agreement with the SM predictions at NNLO QCD $\times$ NLO EW.
References
1 CMS Collaboration Measurement of the $ {\mathrm{W}\mathrm{Z}} $ production cross section in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 7 and 8 TeV and search for anomalous triple gauge couplings at $ \sqrt{s}= $ 8 TeV EPJC 77 (2017) 236 CMS-SMP-14-014
1609.05721
2 ATLAS Collaboration Measurements of $ {\mathrm{W}^{\pm}\mathrm{Z}} $ production cross sections in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 8 TeV with the ATLAS detector and limits on anomalous gauge boson self-couplings PRD 93 (2016) 092004 1603.02151
3 CMS Collaboration Measurement of the $ {\mathrm{W}\mathrm{Z}} $ production cross section in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 13 TeV PLB 766 (2017) 268 CMS-SMP-16-002
1607.06943
4 ATLAS Collaboration Measurement of the $ {\mathrm{W}^{\pm}\mathrm{Z}} $ boson pair-production cross section in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 13 TeV with the ATLAS detector PLB 762 (2016) 1 1606.04017
5 ATLAS Collaboration Measurement of $ {\mathrm{W}^{\pm}\mathrm{Z}} $ production cross sections and gauge boson polarisation in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 13 TeV with the ATLAS detector EPJC 79 (2019) 535 1902.05759
6 CMS Collaboration Measurements of the electroweak diboson production cross sections in proton-proton collisions at $ \sqrt{s}= $ 5.02 TeV using leptonic decays PRL 127 (2021) 191801 CMS-SMP-20-012
2107.01137
7 CMS Collaboration Measurement of the inclusive and differential $ {\mathrm{W}\mathrm{Z}} $ production cross sections, polarization angles, and triple gauge couplings in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 13 TeV JHEP 07 (2022) 032 CMS-SMP-20-014
2110.11231
8 CMS Collaboration HEPData record for this analysis link
9 CMS Collaboration The CMS experiment at the CERN LHC JINST 3 (2008) S08004
10 CMS Collaboration Development of the CMS detector for the CERN LHC \mboxRun 3 JINST 19 (2024) P05064 CMS-PRF-21-001
2309.05466
11 CMS Collaboration Performance of the CMS Level-1 trigger in proton-proton collisions at $ \sqrt{s}= $ 13 TeV JINST 15 (2020) P10017 CMS-TRG-17-001
2006.10165
12 CMS Collaboration The CMS trigger system JINST 12 (2017) P01020 CMS-TRG-12-001
1609.02366
13 CMS Collaboration Performance of the CMS high-level trigger during LHC \mboxRun 2 JINST 19 (2024) P11021 CMS-TRG-19-001
2410.17038
14 P. Nason A new method for combining NLO QCD with shower Monte Carlo algorithms JHEP 11 (2004) 040 hep-ph/0409146
15 S. Frixione, P. Nason, and C. Oleari Matching NLO QCD computations with parton shower simulations: the POWHEG method JHEP 11 (2007) 070 0709.2092
16 S. Alioli, P. Nason, C. Oleari, and E. Re A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG box JHEP 06 (2010) 043 1002.2581
17 T. Melia, P. Nason, R. Röntsch, and G. Zanderighi $ {\mathrm{W^+}\mathrm{W^-}} $, $ {\mathrm{W}\mathrm{Z}} $ and $ {\mathrm{Z}\mathrm{Z}} $ production in the POWHEG box JHEP 11 (2011) 078 1107.5051
18 P. Nason and G. Zanderighi $ {\mathrm{W^+}\mathrm{W^-}} $, $ {\mathrm{W}\mathrm{Z}} $ and $ {\mathrm{Z}\mathrm{Z}} $ production in the POWHEG -box-v2 EPJC 74 (2014) 2702 1311.1365
19 J. Alwall et al. The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations JHEP 07 (2014) 079 1405.0301
20 NNPDF Collaboration Parton distributions from high-precision collider data EPJC 77 (2017) 663 1706.00428
21 C. Bierlich et al. A comprehensive guide to the physics and usage of PYTHIA8.3 SciPost Phys. Codeb. 8 (2022) 2203.11601
22 CMS Collaboration Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements EPJC 80 (2020) 4 CMS-GEN-17-001
1903.12179
23 GEANT4 Collaboration GEANT 4---a simulation toolkit NIM A 506 (2003) 250
24 CMS Collaboration Particle-flow reconstruction and global event description with the CMS detector JINST 12 (2017) P10003 CMS-PRF-14-001
1706.04965
25 CMS Collaboration Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid CMS Technical Proposal CERN-LHCC-2015-010, CMS-TDR-15-02, 2015
link
26 CMS Collaboration Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC JINST 16 (2021) P05014 CMS-EGM-17-001
2012.06888
27 CMS Collaboration Performance of electron reconstruction and selection with the CMS detector in proton-proton collisions at $ \sqrt{s}= $ 8 TeV JINST 10 (2015) P06005 CMS-EGM-13-001
1502.02701
28 CMS Collaboration Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at $ \sqrt{s}= $ 13 TeV JINST 13 (2018) P06015 CMS-MUO-16-001
1804.04528
29 CMS Collaboration Muon identification using multivariate techniques in the CMS experiment in proton-proton collisions at $ \sqrt{s}= $ 13 TeV JINST 19 (2024) P02031 CMS-MUO-22-001
2310.03844
30 M. Cacciari, G. P. Salam, and G. Soyez The anti-$ k_{\mathrm{T}} $ jet clustering algorithm JHEP 04 (2008) 063 0802.1189
31 M. Cacciari, G. P. Salam, and G. Soyez FASTJET user manual EPJC 72 (2012) 1896 1111.6097
32 CMS Collaboration Pileup mitigation at CMS in 13 TeV data JINST 15 (2020) P09018 CMS-JME-18-001
2003.00503
33 D. Bertolini, P. Harris, M. Low, and N. Tran Pileup per particle identification JHEP 10 (2014) 059 1407.6013
34 CMS Collaboration Identification of heavy-flavour jets with the CMS detector in $ {\mathrm{p}\mathrm{p}} $ collisions at 13 TeV JINST 13 (2018) P05011 CMS-BTV-16-002
1712.07158
35 E. Bols et al. Jet flavour classification using DeepJet JINST 15 (2020) P12012 2008.10519
36 CMS Collaboration Performance of missing transverse momentum reconstruction in proton-proton collisions at $ \sqrt{s}= $ 13 TeV using the CMS detector JINST 14 (2019) P07004 CMS-JME-17-001
1903.06078
37 CMS Collaboration Mitigation of anomalous missing transverse momentum measurements in data collected by CMS at $ \sqrt{s}= $ 13 TeV during the LHC \mboxRun 2 Technical Report CMS-DP-2020-018, 2020
CDS
38 ALEPH, DELPHI, L3, OPAL, and SLD Collaborations, LEP Electroweak Working Group, and SLD Electroweak and Heavy Flavour Groups Precision electroweak measurements on the Z resonance Phys. Rept. 427 (2006) 257 hep-ex/0509008
39 CMS Collaboration Observation of single top quark production in association with a Z boson in proton-proton collisions at $ \sqrt{s}= $ 13 TeV PRL 122 (2019) 132003 CMS-TOP-18-008
1812.05900
40 CMS Collaboration Observation of the production of three massive gauge bosons at $ \sqrt{s}= $ 13 TeV PRL 125 (2020) 151802 CMS-SMP-19-014
2006.11191
41 CMS Collaboration Observation of Higgs boson decay to bottom quarks PRL 121 (2018) 121801 CMS-HIG-18-016
1808.08242
42 CMS Collaboration Measurements of inclusive W and Z cross sections in $ {\mathrm{p}\mathrm{p}} $ collisions at $ \sqrt{s}= $ 7 TeV JHEP 01 (2011) 080 CMS-EWK-10-002
1012.2466
43 C. J. Clopper and E. S. Pearson The use of confidence or fiducial limits illustrated in the case of the binomial Biometrika 26 (1934) 404
44 ATLAS Collaboration Measurement of the inelastic proton-proton cross section at $ \sqrt{s}= $ 13 TeV with the ATLAS setector at the LHC PRL 117 (2016) 182002 1606.02625
45 CMS Collaboration Luminosity measurement in proton-proton collisions at 13.6 TeV in 2022 at CMS CMS Physics Analysis Summary, 2024
CMS-PAS-LUM-22-001
CMS-PAS-LUM-22-001
46 CMS Collaboration Precision luminosity measurement in proton-proton collisions at $ \sqrt{s}= $ 13 TeV in 2015 and 2016 at CMS EPJC 81 (2021) 800 CMS-LUM-17-003
2104.01927
47 R. Barlow and C. Beeston Fitting using finite Monte Carlo samples Comput. Phys. Commun. 77 (1993) 219
48 CMS Collaboration The CMS statistical analysis and combination tool: combine Comput. Softw. Big Sci. 8 (2024) 19 CMS-CAT-23-001
2404.06614
49 M. Grazzini et al. NNLO QCD + NLO EW with matrix+OpenLoops: precise predictions for vector-boson pair production JHEP 02 (2020) 087 1912.00068
Compact Muon Solenoid
LHC, CERN