Analysis of the resonant components in ¯¯¯B0→J/ψπ+π−

dc.contributor.authorAbellan Beteta, Carlos
dc.contributor.authorCalvo Gómez, Míriam
dc.contributor.authorCamboni, Alessandro
dc.contributor.authorComerma Montells, Albert
dc.contributor.authorDomingo Bonal, Francesc
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.authorPotterat, Cédric
dc.contributor.authorRives Molina, Vicente José
dc.contributor.authorRuiz, Hugo (Ruiz Pérez)
dc.contributor.authorVázquez Gómez, Ricard
dc.contributor.authorVilasis-Cardona, Xavier
dc.contributor.authorLHCb Collaboration
dc.date.accessioned2019-04-08T12:00:24Z
dc.date.available2019-04-08T12:00:24Z
dc.date.issued2013-03-01
dc.date.updated2019-04-08T12:00:25Z
dc.description.abstractInterpretation of C P violation measurements using charmonium decays, in both the ¯¯¯ B 0 and ¯¯¯ B 0 s systems, can be subject to changes due to "penguin" type diagrams. These effects can be investigated using measurements of the Cabibbo-suppressed ¯¯¯ B 0 → J / ψ π + π − decays. The final state composition of this channel is investigated using a 1.0     fb − 1 sample of data produced in 7 TeV p p collisions at the LHC and collected by the LHCb experiment. A modified Dalitz-plot analysis is performed using both the invariant mass spectra and the decay angular distributions. An improved measurement of the ¯¯¯ B 0 → J / ψ π + π − branching fraction of ( 3.97 ± 0.09 ± 0.11 ± 0.16 ) × 10 − 5 is reported where the first uncertainty is statistical, the second is systematic, and the third is due to the uncertainty of the branching fraction of the decay B − → J / ψ K − used as a normalization channel. Significant production of f 0 ( 500 ) and ρ ( 770 ) resonances is found in the substructure of the J / ψ π + π − final state, and this indicates that they are viable final states for C P violation studies. In contrast evidence for the f 0 ( 980 ) resonance is not found. This allows us to establish the first upper limit on the branching fraction product B ( ¯¯¯ B 0 → J / ψ f 0 ( 980 ) ) × B ( f 0 ( 980 ) → π + π − ) < 1.1 × 10 − 6 , leading to an upper limit on the absolute value of the mixing angle of the f 0 ( 980 ) with the f 0 ( 500 ) of less than 31°, both at 90% confidence level.
dc.format.extent21 p.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec622090
dc.identifier.issn1550-7998
dc.identifier.urihttps://hdl.handle.net/2445/131790
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.1103/PhysRevD.87.052001
dc.relation.ispartofPhysical Review D, 2013, vol. 87, num. 11, p. 052001
dc.relation.urihttps://doi.org/10.1103/PhysRevD.87.052001
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.titleAnalysis of the resonant components in ¯¯¯B0→J/ψπ+π−
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/publishedVersion

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