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dc.contributor.authorKhachatryan, Vladimir
dc.contributor.authorBrochero Cifuentes, Javier Andrés 
dc.contributor.authorCabrillo Bartolomé, José Iban 
dc.contributor.authorCalderón Tazón, Alicia 
dc.contributor.authorDuarte Campderros, Jorge 
dc.contributor.authorFernández García, Marcos 
dc.contributor.authorGómez Gramuglio, Gervasio 
dc.contributor.authorGonzález Sánchez, Francisco Javier 
dc.contributor.authorGraziano, Alberto
dc.contributor.authorLópez Virto, María Amparo
dc.contributor.authorMarco de Lucas, Jesús 
dc.contributor.authorMarco de Lucas, Rafael José
dc.contributor.authorMartínez Rivero, Celso
dc.contributor.authorMatorras Weinig, Francisco 
dc.contributor.authorMuñoz Sánchez, Francisca Javiela
dc.contributor.authorPiedra Gómez, Jonatan 
dc.contributor.authorRodrigo Anoro, Teresa 
dc.contributor.authorRodríguez Marrero, Ana Yaiza
dc.contributor.authorRuiz Jimeno, Alberto 
dc.contributor.authorScodellaro, Luca 
dc.contributor.authorVila Álvarez, Iván  
dc.contributor.authorVilar Cortabitarte, Rocío 
dc.contributor.otherUniversidad de Cantabriaes_ES
dc.date.accessioned2018-06-19T11:29:30Z
dc.date.available2018-06-19T11:29:30Z
dc.date.issued2014-09
dc.identifier.issn0370-2693
dc.identifier.issn1873-2445
dc.identifier.otherFPA2014-55295-C3-1-R
dc.identifier.otherFPA 2011-28694-C02-01
dc.identifier.urihttp://hdl.handle.net/10902/13962
dc.description.abstractThe ratio of the top-quark branching fractions R = ß(t→Wb)/ß(t →Wq), where the denominator includes the sum over all down-type quarks (q =b, s, d), is measured in the t¯t dilepton final state with proton–proton collision data at vs=8TeVfrom an integrated luminosity of 19.7fb-1, collected with the CMS detector. In order to quantify the purity of the signal sample, the cross section is measured by fitting the observed jet multiplicity, thereby constraining the signal and background contributions. By counting the number of b jets per event, an unconstrained value of R =1.014 ± 0.003 (stat.) ± 0.032 (syst.)is measured, in a good agreement with current precision measurements in electroweak and flavour sectors. A lower limit R >0.955at the 95% confidence level is obtained after requiring R =1, and a lower limit on the Cabibbo–Kobayashi–Maskawa matrix element |Vtb| >0.975 is set at 95% confidence level. The result is combined with a previous CMS measurement of the t-channel single-top-quark cross section to determine the top-quark total decay width, Gt=1.36 ± 0.02 (stat.) + 0.14-0.11 (syst.) GeV.es_ES
dc.format.extent25 p.es_ES
dc.language.isoenges_ES
dc.publisherElsevieres_ES
dc.rightsAtribución 3.0 España*
dc.rights.urihttp://creativecommons.org/licenses/by/3.0/es/*
dc.sourcePhysics Letters B, Vol. 736, Pp. 33–57, (2014)es_ES
dc.titleMeasurement of the ratio ß(t→Wb)/ß(t →Wq) in pp collisions at vs = 8 TeVes_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.relation.publisherVersionhttps://doi.org/10.1016/j.physletb.2014.06.076es_ES
dc.rights.accessRightsopenAccesses_ES
dc.identifier.DOI10.1016/j.physletb.2014.06.076
dc.type.versionpublishedVersiones_ES


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Atribución 3.0 EspañaExcepto si se señala otra cosa, la licencia del ítem se describe como Atribución 3.0 España