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 fnal states and a simultaneous likelihood ft to the number of events in four diferent lepton favour categories: eee, eeµ, µµe, and µµµ. The selection is optimized to minimize the number of background events, and relies on an efcient prompt lepton discrimination strategy. The WZ production cross section is measured in a phase space defned within a 30 GeV window around the Z boson mass, as σtotal(pp → WZ) = 55.2±1.2 (stat)±1.2 (syst)±0.8 (lumi)±0.3 (theo) pb. In addition, the cross section is measured in a fducial phase space closer to the detector level requirements. All the measurements presented in this paper are in agreement with standard model predictions
Measurement of the inclusive WZ production cross section in pp collisions at sqrt(s) = 13.6 TeV
BABBAR, J.;CANDELISE, V.;DELLA RICCA, G.;
2025-01-01
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 fnal states and a simultaneous likelihood ft to the number of events in four diferent lepton favour categories: eee, eeµ, µµe, and µµµ. The selection is optimized to minimize the number of background events, and relies on an efcient prompt lepton discrimination strategy. The WZ production cross section is measured in a phase space defned within a 30 GeV window around the Z boson mass, as σtotal(pp → WZ) = 55.2±1.2 (stat)±1.2 (syst)±0.8 (lumi)±0.3 (theo) pb. In addition, the cross section is measured in a fducial phase space closer to the detector level requirements. All the measurements presented in this paper are in agreement with standard model predictionsFile | Dimensione | Formato | |
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JHEP04(2025)115.pdf
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