Measurement of the W ± Z boson pair-production cross section in pp collisions at s=13 TeV with the ATLAS detector

The production of W ± Z events in proton–proton collisions at a centre-of-mass energy of 13 TeV is measured with the ATLAS detector at the LHC. The collected data correspond to an integrated luminosity of 3.2 fb −1 . The W ± Z candidates are reconstructed using leptonic decays of the gauge bosons in...

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Publicado: 2016
Acceso en línea:https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_03702693_v762_n_p1_Aaboud
http://hdl.handle.net/20.500.12110/paper_03702693_v762_n_p1_Aaboud
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spelling paper:paper_03702693_v762_n_p1_Aaboud2023-06-08T15:37:29Z Measurement of the W ± Z boson pair-production cross section in pp collisions at s=13 TeV with the ATLAS detector The production of W ± Z events in proton–proton collisions at a centre-of-mass energy of 13 TeV is measured with the ATLAS detector at the LHC. The collected data correspond to an integrated luminosity of 3.2 fb −1 . The W ± Z candidates are reconstructed using leptonic decays of the gauge bosons into electrons or muons. The measured inclusive cross section in the detector fiducial region for leptonic decay modes is σ W ± Z→ℓ ′ νℓℓ fid. =63.2±3.2(stat.)±2.6(sys.)±1.5(lumi.) fb. In comparison, the next-to-leading-order Standard Model prediction is 53.4 −2.8 +3.6 fb. The extrapolation of the measurement from the fiducial to the total phase space yields σ W ± Z tot. =50.6±2.6(stat.)±2.0(sys.)±0.9(th.)±1.2(lumi.) pb, in agreement with a recent next-to-next-to-leading-order calculation of 48.2 −1.0 +1.1 pb. The cross section as a function of jet multiplicity is also measured, together with the charge-dependent W + Z and W − Z cross sections and their ratio. © 2016 The Author(s) 2016 https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_03702693_v762_n_p1_Aaboud http://hdl.handle.net/20.500.12110/paper_03702693_v762_n_p1_Aaboud
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
description The production of W ± Z events in proton–proton collisions at a centre-of-mass energy of 13 TeV is measured with the ATLAS detector at the LHC. The collected data correspond to an integrated luminosity of 3.2 fb −1 . The W ± Z candidates are reconstructed using leptonic decays of the gauge bosons into electrons or muons. The measured inclusive cross section in the detector fiducial region for leptonic decay modes is σ W ± Z→ℓ ′ νℓℓ fid. =63.2±3.2(stat.)±2.6(sys.)±1.5(lumi.) fb. In comparison, the next-to-leading-order Standard Model prediction is 53.4 −2.8 +3.6 fb. The extrapolation of the measurement from the fiducial to the total phase space yields σ W ± Z tot. =50.6±2.6(stat.)±2.0(sys.)±0.9(th.)±1.2(lumi.) pb, in agreement with a recent next-to-next-to-leading-order calculation of 48.2 −1.0 +1.1 pb. The cross section as a function of jet multiplicity is also measured, together with the charge-dependent W + Z and W − Z cross sections and their ratio. © 2016 The Author(s)
title Measurement of the W ± Z boson pair-production cross section in pp collisions at s=13 TeV with the ATLAS detector
spellingShingle Measurement of the W ± Z boson pair-production cross section in pp collisions at s=13 TeV with the ATLAS detector
title_short Measurement of the W ± Z boson pair-production cross section in pp collisions at s=13 TeV with the ATLAS detector
title_full Measurement of the W ± Z boson pair-production cross section in pp collisions at s=13 TeV with the ATLAS detector
title_fullStr Measurement of the W ± Z boson pair-production cross section in pp collisions at s=13 TeV with the ATLAS detector
title_full_unstemmed Measurement of the W ± Z boson pair-production cross section in pp collisions at s=13 TeV with the ATLAS detector
title_sort measurement of the w ± z boson pair-production cross section in pp collisions at s=13 tev with the atlas detector
publishDate 2016
url https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_03702693_v762_n_p1_Aaboud
http://hdl.handle.net/20.500.12110/paper_03702693_v762_n_p1_Aaboud
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