First observations of B¯s0→D+D-, Ds+D- and D0D¯0 decays

dc.contributor.authorCamboni, Alessandro
dc.contributor.authorComerma Montells, Albert
dc.contributor.authorGarrido Beltrán, Lluís
dc.contributor.authorGraciani Díaz, Ricardo
dc.contributor.authorGraugés Pous, Eugeni
dc.contributor.authorLópez Asamar, Elias
dc.contributor.authorPérez-Calero Yzquierdo, Antonio
dc.contributor.authorPicatoste Olloqui, Eduardo
dc.contributor.authorPotterat, Cédric
dc.contributor.authorRives Molina, Vicente José
dc.contributor.authorRuiz, Hugo (Ruiz Pérez)
dc.contributor.authorVázquez Gómez, Ricard
dc.contributor.authorAbellan Beteta, Carlos
dc.contributor.authorCalvo Gómez, Míriam
dc.contributor.authorOyanguren Campos, Arantza de
dc.contributor.authorRuiz Valls, Pablo
dc.contributor.authorVilasis-Cardona, Xavier
dc.contributor.authorLHCb Collaboration
dc.date.accessioned2019-04-08T13:48:42Z
dc.date.available2019-04-08T13:48:42Z
dc.date.issued2013-05-01
dc.date.updated2019-04-08T13:48:43Z
dc.description.abstractFirst observations and measurements of the branching fractions of the ¯¯¯ B 0 s → D + D − , ¯¯¯ B 0 s → D + s D − and ¯¯¯ B 0 s → D 0 ¯¯¯ D 0 decays are presented using 1.0     fb − 1 of data collected by the LHCb experiment. These branching fractions are normalized to those of ¯¯¯ B 0 → D + D − , B 0 → D − D + s and B − → D 0 D − s , respectively. An excess of events consistent with the decay ¯¯¯ B 0 → D 0 ¯¯¯ D 0 is also seen, and its branching fraction is measured relative to that of B − → D 0 D − s . Improved measurements of the branching fractions B ( ¯¯¯ B 0 s → D + s D − s ) and B ( B − → D 0 D − s ) are reported, each relative to B ( B 0 → D − D + s ) . The ratios of branching fractions are B ( ¯¯¯ B 0 s → D + D − ) B ( ¯¯¯ B 0 → D + D − ) = 1.08 ± 0.20 ± 0.10 , B ( ¯¯¯ B 0 s → D + s D − ) B ( B 0 → D − D + s ) = 0.050 ± 0.008 ± 0.004 , B ( ¯¯¯ B 0 s → D 0 ¯¯¯ D 0 ) B ( B − → D 0 D − s ) = 0.019 ± 0.003 ± 0.003 , B ( ¯¯¯ B 0 → D 0 ¯¯¯ D 0 ) B ( B − → D 0 D − s ) < 0.0024 at 90% CL, B ( ¯¯¯ B 0 s → D + s D − s ) B ( B 0 → D − D + s ) = 0.56 ± 0.03 ± 0.04 , B ( B − → D 0 D − s ) B ( B 0 → D − D + s ) = 1.22 ± 0.02 ± 0.07 , where the uncertainties are statistical and systematic, respectively.
dc.format.extent12 p.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec628984
dc.identifier.issn1550-7998
dc.identifier.urihttps://hdl.handle.net/2445/131837
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.1103/PhysRevD.87.092007
dc.relation.ispartofPhysical Review D, 2013, vol. 87, num. 9, p. 092007
dc.relation.urihttps://doi.org/10.1103/PhysRevD.87.092007
dc.rightscc by (c) CERN; LHCb Collaboration, 2013
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess
dc.rights.urihttp://creativecommons.org/licenses/by/3.0/es/
dc.sourceArticles publicats en revistes (Física Quàntica i Astrofísica)
dc.subject.classificationFísica de partícules
dc.subject.classificationExperiments
dc.subject.otherParticle physics
dc.subject.otherExperiments
dc.titleFirst observations of B¯s0→D+D-, Ds+D- and D0D¯0 decays
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/publishedVersion

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