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dc.contributor.authorAad, G.
dc.contributor.authorRodríguez Chala, Mikael 
dc.contributor.authorAtlas Collaboration
dc.date.accessioned2024-11-18T09:19:41Z
dc.date.available2024-11-18T09:19:41Z
dc.date.issued2024-03-25
dc.identifier.citationAad, G. & Rodríguez Chala, M. & ATLAS Collaboration. et. al. Eur. Phys. J. C (2024) 84:315. [https://doi.org/10.1140/epjc/s10052-024-12438-w]es_ES
dc.identifier.urihttps://hdl.handle.net/10481/96989
dc.description.abstractThis paper presents for the first time a precise measurement of the production properties of the Z boson in the full phase space of the decay leptons. This is in contrast to the many previous precise unfolded measurements performed in the fiducial phase space of the decay leptons. The measurement is obtained from proton–proton collision data collected by the ATLAS experiment in 2012 at √ s = 8 TeV at the LHC and corresponding to an integrated luminosity of 20.2 fb−1. The results, based on a total of 15.3 million Zboson decays to electron and muon pairs, extend and improve a previous measurement of the full set of angular coefficients describing Z-boson decay. The double-differential crosssection distributions in Z-boson transverse momentum pT and rapidity y are measured in the pole region, defined as 80 < m < 100 GeV, over the range |y| < 3.6. The total uncertainty of the normalised cross-section measurements in the peak region of the pT distribution is dominated by statistical uncertainties over the full range and increases as a function of rapidity from 0.5–1.0% for |y| < 2.0 to 2 − 7% at higher rapidities. The results for the rapidity-dependent transverse momentum distributions are compared to stateof- the-art QCD predictions, which combine in the best cases approximateN4LL resummationwithN3LO fixed-order perturbative calculations. The differential rapidity distributions integrated over pT are even more precise, with accuracies from 0.2–0.3% for |y| < 2.0 to 0.4–0.9% at higher rapidities, and are compared to fixed-order QCD predictions using the most recent parton distribution functions. The agreement between data and predictions is quite good in most cases.es_ES
dc.description.sponsorshipCERN for the very successful operation of the LHCes_ES
dc.description.sponsorshipANPCyT, Argentinaes_ES
dc.description.sponsorshipYerPhI, Armeniaes_ES
dc.description.sponsorshipARC, Australiaes_ES
dc.description.sponsorshipBMWFW and FWF, Austriaes_ES
dc.description.sponsorshipANAS, Azerbaijanes_ES
dc.description.sponsorshipCNPq and FAPESP, Braziles_ES
dc.description.sponsorshipNSERC, NRC and CFI, Canadaes_ES
dc.description.sponsorshipANID, Chilees_ES
dc.description.sponsorshipCAS, MOST and NSFC, Chinaes_ES
dc.description.sponsorshipMinciencias, Colombiaes_ES
dc.description.sponsorshipMEYS CR, Czech Republices_ES
dc.description.sponsorshipDNRF and DNSRC, Denmarkes_ES
dc.description.sponsorshipIN2P3-CNRS and CEA-DRF/IRFU, Francees_ES
dc.description.sponsorshipSRNSFG, Georgiaes_ES
dc.description.sponsorshipBMBF, HGF and MPG, Germanyes_ES
dc.description.sponsorshipGSRI, Greecees_ES
dc.description.sponsorshipRGC and Hong Kong SAR, Chinaes_ES
dc.description.sponsorshipISF and Benoziyo Center, Israeles_ES
dc.description.sponsorshipINFN, Italyes_ES
dc.description.sponsorshipMEXT and JSPS, Japanes_ES
dc.description.sponsorshipCNRST, Moroccoes_ES
dc.description.sponsorshipNWO,Netherlandses_ES
dc.description.sponsorshipRCN,Norwayes_ES
dc.description.sponsorshipMEiN, Polandes_ES
dc.description.sponsorshipFCT, Portugales_ES
dc.description.sponsorshipMNE/IFA, Romaniaes_ES
dc.description.sponsorshipMESTD, Serbiaes_ES
dc.description.sponsorshipMSSR, Slovakiaes_ES
dc.description.sponsorshipARRS and MIZŠ, Sloveniaes_ES
dc.description.sponsorshipDSI/NRF, South Africaes_ES
dc.description.sponsorshipMICINN, Spaines_ES
dc.description.sponsorshipSRC and Wallenberg Foundation, Swedenes_ES
dc.description.sponsorshipSERI, SNSF and Cantons of Bern and Geneva, Switzerlandes_ES
dc.description.sponsorshipMOST, Taiwanes_ES
dc.description.sponsorshipTENMAK, Türkiyees_ES
dc.description.sponsorshipSTFC, United Kingdomes_ES
dc.description.sponsorshipDOE and NSF, United States of Americaes_ES
dc.description.sponsorshipBCKDF, CANARIE, Compute Canada and CRC, Canadaes_ES
dc.description.sponsorshipPRIMUS 21/SCI/017 and UNCE SCI/013, Czech Republices_ES
dc.description.sponsorshipCOST, ERC, ERDF, Horizon 2020 and Marie Skłodowska-Curie Actions, European Uniones_ES
dc.description.sponsorshipInvestissements d’Avenir Labex, Investissements d’Avenir Idex and ANR,Francees_ES
dc.description.sponsorshipDFGandAvHFoundation, Germanyes_ES
dc.description.sponsorshipHerakleitos, Thales and Aristeia programmes co-financed by EU-ESF and the Greek NSRF, Greecees_ES
dc.description.sponsorshipBSF-NSF and MINERVA, Israeles_ES
dc.description.sponsorshipNorwegian Financial Mechanism 2014-2021, Norwayes_ES
dc.description.sponsorshipNCN and NAWA, Polandes_ES
dc.description.sponsorshipLa Caixa Banking Foundation, CERCA Programme Generalitat de Catalunya and PROMETEO and GenT Programmes Generalitat Valenciana, Spaines_ES
dc.description.sponsorshipGöran Gustafssons Stiftelse, Swedenes_ES
dc.description.sponsorshipThe Royal Society and Leverhulme Trust, United Kingdomes_ES
dc.description.sponsorshipCrucial computing support from all WLCG partnerses_ES
dc.language.isoenges_ES
dc.publisherSpringer Naturees_ES
dc.rightsAtribución 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.titleA precise measurement of the Z-boson double-differential transverse momentum and rapidity distributions in the full phase space of the decay leptons with the ATLAS experiment at √ s = 8 TeVes_ES
dc.typejournal articlees_ES
dc.rights.accessRightsopen accesses_ES
dc.identifier.doi10.1140/epjc/s10052-024-12438-w
dc.type.hasVersionVoRes_ES


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