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dc.contributor.authorAad, G.
dc.contributor.authorAguilar Saavedra, Juan Antonio 
dc.contributor.authorAtlas Collaboration, /
dc.date.accessioned2024-10-16T11:15:33Z
dc.date.available2024-10-16T11:15:33Z
dc.date.issued2016-03-17
dc.identifier.citationAad, G. & Rodríguez Chala, R. & Atlas Collaboration. J. High Energ. Phys. 2016, 127 (2016). [https://doi.org/10.1007/JHEP03(2016)127]es_ES
dc.identifier.urihttps://hdl.handle.net/10481/96021
dc.description.abstractharged Higgs bosons heavier than the top quark and decaying via H ± → tb are searched for in proton-proton collisions measured with the ATLAS experiment at √s=8 TeV corresponding to an integrated luminosity of 20.3fb−1. The production of a charged Higgs boson in association with a top quark, gb → tH ±, is explored in the mass range 200 to 600 GeV using multi-jet final states with one electron or muon. In order to separate the signal from the Standard Model background, analysis techniques combining several kinematic variables are employed. An excess of events above the background-only hypothesis is observed across a wide mass range, amounting to up to 2.4 standard deviations. Upper limits are set on the gb → tH ± production cross section times the branching fraction BR(H ± → tb). Additionally, the complementary s-channel production, qq ′ → H ±, is investigated through a reinterpretation of W ′ → tb searches in ATLAS. Final states with one electron or muon are relevant for H ± masses from 0.4 to 2.0 TeV, whereas the all-hadronic final state covers the range 1.5 to 3.0 TeV. In these search channels, no significant excesses from the predictions of the Standard Model are observed, and upper limits are placed on the qq ′ → H ± production cross section times the branching fraction BR(H ± → tb).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.sponsorshipSSTC, Belaruses_ES
dc.description.sponsorshipCNPq and FAPESP, Braziles_ES
dc.description.sponsorshipNSERC, NRC and CFI, Canadaes_ES
dc.description.sponsorshipCONICYT, Chilees_ES
dc.description.sponsorshipCAS, MOST and NSFC, Chinaes_ES
dc.description.sponsorshipCOLCIENCIAS, Colombiaes_ES
dc.description.sponsorshipMSMT CR, MPO CR and VSC CR, Czech Republices_ES
dc.description.sponsorshipDNRF, DNSRC and Lundbeck Foundation, Denmarkes_ES
dc.description.sponsorshipIN2P3-CNRS, CEADSM/ IRFU, Francees_ES
dc.description.sponsorshipGNSF, Georgiaes_ES
dc.description.sponsorshipBMBF, HGF, and MPG, Germanyes_ES
dc.description.sponsorshipGSRT, Greecees_ES
dc.description.sponsorshipRGC, Hong Kong SAR, Chinaes_ES
dc.description.sponsorshipISF, I-CORE and Benoziyo Center, Israeles_ES
dc.description.sponsorshipINFN, Italyes_ES
dc.description.sponsorshipMEXT and JSPS, Japanes_ES
dc.description.sponsorshipCNRST, Moroccoes_ES
dc.description.sponsorshipFOM and NWO, Netherlandses_ES
dc.description.sponsorshipRCN, Norwayes_ES
dc.description.sponsorshipMNiSW and NCN, Polandes_ES
dc.description.sponsorshipFCT, Portugales_ES
dc.description.sponsorshipMNE/IFA, Romaniaes_ES
dc.description.sponsorshipof Russia and NRC KI, Russian Federationes_ES
dc.description.sponsorshipJINR; MESTD, Serbiaes_ES
dc.description.sponsorshipMSSR, Slovakiaes_ES
dc.description.sponsorshipARRS and MIZ S, Sloveniaes_ES
dc.description.sponsorshipDST/NRF, South Africaes_ES
dc.description.sponsorshipMINECO, 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.sponsorshipThe Canada Council, CANARIE, CRC, Compute Canada, FQRNT, and the Ontario Innovation Trust, Canadaes_ES
dc.description.sponsorshipEPLANET, ERC, FP7, Horizon 2020 and Marie Sk lodowska-Curie Actions, European Uniones_ES
dc.description.sponsorshipInvestissements d'Avenir Labex and Idex, ANR, Region Auvergne and Fondation Partager le Savoir, Francees_ES
dc.description.sponsorshipDFG and AvH Foundation, Germanyes_ES
dc.description.sponsorshipHerakleitos, Thales and Aristeia programmes co- nanced by EU-ESF and the Greek NSRFes_ES
dc.description.sponsorshipBSF, GIF and Minerva, Israeles_ES
dc.description.sponsorshipBRF, Norwayes_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.publisherSpringeres_ES
dc.rightsAtribución 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.subjectHadron-Hadron scatteringes_ES
dc.subjectHiggs physicses_ES
dc.titleSearch for charged Higgs bosons in the H ± → tb decay channel in pp collisions at √s=8 TeV using the ATLAS detectores_ES
dc.typejournal articlees_ES
dc.rights.accessRightsopen accesses_ES
dc.identifier.doi10.1007/JHEP03(2016)127
dc.type.hasVersionVoRes_ES


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