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dc.contributor.authorAad, G.
dc.contributor.authorAguilar Saavedra, Juan Antonio 
dc.contributor.authorRodríguez Chala, Mikael 
dc.contributor.authorAtlas Collaboration
dc.date.accessioned2022-12-13T12:12:24Z
dc.date.available2022-12-13T12:12:24Z
dc.date.issued2022-11-09
dc.identifier.citationThe ATLAS collaboration... [et al.]. Measurement of the polarisation of single top quarks and antiquarks produced in the t-channel at s√ = 13 TeV and bounds on the tWb dipole operator from the ATLAS experiment. J. High Energ. Phys. 2022, 40 (2022). [https://doi.org/10.1007/JHEP11(2022)040]es_ES
dc.identifier.urihttps://hdl.handle.net/10481/78425
dc.description.abstractA simultaneous measurement of the three components of the top-quark and top-antiquark polarisation vectors in t-channel single-top-quark production is presented. This analysis is based on data from proton-proton collisions at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 139 fb(-1), collected with the ATLAS detector at the LHC. Selected events contain exactly one isolated electron or muon, large missing transverse momentum and exactly two jets, one being b-tagged. Stringent selection requirements are applied to discriminate t-channel single-top-quark events from the background contributions. The top-quark and top-antiquark polarisation vectors are measured from the distributions of the direction cosines of the charged-lepton momentum in the top-quark rest frame. The three components of the polarisation vector for the selected top-quark event sample are P-x' = 0.01 +/- 0.18, P-y' = -0.029 +/- 0.027, P-z' = 0.91 +/- 0.10 and for the top-antiquark event sample they are P-x' = -0.02 +/- 0.20, P-y' = -0.007 +/- 0.051, P-z' = -0.79 +/- 0.16. Normalised differential cross-sections corrected to a fiducial region at the stable-particle level are presented as a function of the charged-lepton angles for top-quark and top-antiquark events inclusively and separately. These measurements are in agreement with Standard Model predictions. The angular differential cross-sections are used to derive bounds on the complex Wilson coefficient of the dimension-six O-tW operator in the framework of an effective field theory. The obtained bounds are C-tW is an element of[-0.9, 1.4] and C-itW is an element of [-0.8, 0.2], both at 95% confidence level.es_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.sponsorshipSSTC, Belaruses_ES
dc.description.sponsorshipCNPq and FAPESP, Braziles_ES
dc.description.sponsorshipNSERC, NRC and CFI, Canadaes_ES
dc.description.sponsorshipCERNes_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, Portugaes_ES
dc.description.sponsorshipMNE/IFA, Romaniaes_ES
dc.description.sponsorshipJINRes_ES
dc.description.sponsorshipMES of Russia and NRC KI, Russian Federationes_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.sponsorshipTAEK, Turkeyes_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.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.sponsorshipDFG and AvH Foundation, 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 GIF, 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.language.isoenges_ES
dc.publisherSpringeres_ES
dc.rightsAtribución 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.subjectHadron-Hadron scatteringes_ES
dc.subjectTop physicses_ES
dc.titleMeasurement of the polarisation of single top quarks and antiquarks produced in the t-channel at s√ = 13 TeV and bounds on the tWb dipole operator from the ATLAS experimentes_ES
dc.typejournal articlees_ES
dc.rights.accessRightsopen accesses_ES
dc.identifier.doi10.1007/JHEP11(2022)040
dc.type.hasVersionVoRes_ES


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