{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.155693.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2855546"}},{"@id":"https://doi.org/10.1007/JHEP04(2025)115","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2024","description":"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: eee, ee$\\mu$, $\\mu\\mu $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 $\\sigma_{\\text{total}}$(pp $\\to$ WZ) = 55.2 $\\pm$ 1.2 (stat) $\\pm$ 1.2 (syst) $\\pm$ 0.8 (lumi) $\\pm$ 0.3 (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.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.155693.v1/t1","@type":"Dataset","description":"Number of events for the different lepton flavour categories in the ZZ control region accounting for the fit to data....","name":"Figure 2a"},{"@id":"https://doi.org/10.17182/hepdata.155693.v1/t2","@type":"Dataset","description":"Number of events for the different lepton flavour categories in the ttZ control region accounting for the fit to data....","name":"Figure 4a"},{"@id":"https://doi.org/10.17182/hepdata.155693.v1/t3","@type":"Dataset","description":"Number of events for the different lepton flavour categories in the X+#gamma control region accounting for the fit to data....","name":"Figure 5a"},{"@id":"https://doi.org/10.17182/hepdata.155693.v1/t4","@type":"Dataset","description":"Number of events for the different lepton flavour categories in the signal region accounting for the fit to data. The...","name":"Figure 6a"},{"@id":"https://doi.org/10.17182/hepdata.155693.v1/t5","@type":"Dataset","description":"Sum of the charge of the final-state leptons in the signal region accounting for the fit to data. This distribution...","name":"Figure 7a"},{"@id":"https://doi.org/10.17182/hepdata.155693.v1/t6","@type":"Dataset","description":"Invariant mass of the trilepton system in the signal region accounting for the fit to data. This distribution is not...","name":"Figure 7d"},{"@id":"https://doi.org/10.17182/hepdata.155693.v1/t7","@type":"Dataset","description":"Measured fiducial cross sections and their corresponding uncertainties for the flavourexclusive and flavour-inclusive categories. The predictions from both POWHEG at...","name":"Fiducial cross section"},{"@id":"https://doi.org/10.17182/hepdata.155693.v1/t8","@type":"Dataset","description":"Total WZ production cross section for each of the flavour-exclusive and for the flavour-inclusive categories. The vertical bands show different...","name":"Total cross section"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2855546?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/155693"}],"inLanguage":"en","name":"Measurement of the inclusive WZ production cross section in pp collisions at $\\sqrt{s}$ = 13.6 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2855546?version=1","version":1}