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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.accessioned2022-09-23T11:42:05Z
dc.date.available2022-09-23T11:42:05Z
dc.date.issued2022-08-18
dc.identifier.citationAad, G... [et al.]. Direct constraint on the Higgs–charm coupling from a search for Higgs boson decays into charm quarks with the ATLAS detector. Eur. Phys. J. C 82, 717 (2022). [https://doi.org/10.1140/epjc/s10052-022-10588-3]es_ES
dc.identifier.urihttps://hdl.handle.net/10481/76914
dc.description.abstractA search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton– proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of √ s = 13 TeV and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb−1. Flavourtagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW,WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the (W/Z)Z(→ c ¯ c) process and 3.8 (4.6) standard deviations for the (W/Z)W(→ cq) process. The (W/Z)H(→ c ¯ c) search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model crosssection times branching fraction for a Higgs boson with a mass of 125 GeV, corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier |κc| < 8.5 (12.4), at the 95% confidence level. A combination with theATLAS(W/Z)H, H → b¯b analysis is performed, allowing the ratio κc/κb to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level.es_ES
dc.description.sponsorshipANPCyT, Argentinaes_ES
dc.description.sponsorshipYerPhI, Armeniaes_ES
dc.description.sponsorshipARC, Australiaes_ES
dc.description.sponsorshipBMWFWandFWF,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.sponsorshipCERN; ANID, 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 andMPG, 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.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, USAes_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.sponsorshipBSFNSF and GIF, Israeles_ES
dc.description.sponsorshipNorwegian FinancialMechanism 2014-2021, Norwayes_ES
dc.description.sponsorshipNCNandNAWA, 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, UK.es_ES
dc.language.isoenges_ES
dc.publisherSpringeres_ES
dc.rightsAtribución 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.titleDirect constraint on the Higgs–charm coupling from a search for Higgs boson decays into charm quarks with the ATLAS detectores_ES
dc.typejournal articlees_ES
dc.rights.accessRightsopen accesses_ES
dc.identifier.doi10.1140/epjc/s10052-022-10588-3
dc.type.hasVersionVoRes_ES


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