Measurement of the resonant and CP components in ¯¯B0 → J/ψπ+π− decays

dc.contributor.authorBadalov, Alexey
dc.contributor.authorCalvo Gómez, Míriam
dc.contributor.authorCamboni, Alessandro
dc.contributor.authorGarrido Beltrán, Lluís
dc.contributor.authorGraciani Díaz, Ricardo
dc.contributor.authorGraugés Pous, Eugeni
dc.contributor.authorMarin Benito, Carla
dc.contributor.authorPicatoste Olloqui, Eduardo
dc.contributor.authorRives Molina, Vicente José
dc.contributor.authorRuiz, Hugo (Ruiz Pérez)
dc.contributor.authorVilasis-Cardona, Xavier
dc.contributor.authorLHCb Collaboration
dc.date.accessioned2019-04-02T11:31:29Z
dc.date.available2019-04-02T11:31:29Z
dc.date.issued2014-07-09
dc.date.updated2019-04-02T11:31:29Z
dc.description.abstractThe resonant structure of the reaction ¯ B 0 → J / ψ π + π − is studied using data from 3     fb − 1 of integrated luminosity collected by the LHCb experiment, one third at 7 TeV center-of-mass energy and the remainder at 8 TeV. The invariant mass of the π + π − pair and three decay angular distributions are used to determine the fractions of the resonant and nonresonant components. Six interfering π + π − states, ρ ( 770 ) , f 0 ( 500 ) , f 2 ( 1270 ) , ρ ( 1450 ) , ω ( 782 ) and ρ ( 1700 ) , are required to give a good description of invariant mass spectra and decay angular distributions. The positive and negative charge parity fractions of each of the resonant final states are determined. The f 0 ( 980 ) meson is not seen and the upper limit on its presence, compared with the observed f 0 ( 500 ) rate, is inconsistent with a model where these scalar mesons are formed from two quarks and two antiquarks (tetraquarks) at the eight standard deviation level. In the q ¯ q model, the absolute value of the mixing angle between the f 0 ( 980 ) and the f 0 ( 500 ) scalar mesons is limited to be less than 17° at 90% confidence level.
dc.format.extent21 p.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec645756
dc.identifier.issn1550-7998
dc.identifier.urihttps://hdl.handle.net/2445/131206
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.1103/PhysRevD.90.012003
dc.relation.ispartofPhysical Review D, 2014, vol. 90, num. 1, p. 012003
dc.relation.urihttps://doi.org/10.1103/PhysRevD.90.012003
dc.rightscc by (c) CERN; LHCb Collaboration, 2014
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.classificationGran Col·lisionador d'Hadrons
dc.subject.classificationRessonància
dc.subject.classificationExperiments
dc.subject.otherParticle physics
dc.subject.otherLarge Hadron Collider (France and Switzerland)
dc.subject.otherResonance
dc.subject.otherExperiments
dc.titleMeasurement of the resonant and CP components in ¯¯B0 → J/ψπ+π− decays
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/publishedVersion

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