Angular analysis of B0→D∗−D∗+s with D∗+s→D+sγ decays

dc.contributor.authorLHCb Collaboration
dc.contributor.authorAlfonso Albero, Alejandro
dc.contributor.authorGarcía Moreno, Paula
dc.contributor.authorGarrido Beltrán, Lluís
dc.contributor.authorGironella Gironell, P.
dc.contributor.authorGomez Fernandez, S.
dc.contributor.authorGraugés Pous, Eugeni
dc.contributor.authorLobo Salvia, A.
dc.contributor.authorMauricio, J.
dc.contributor.authorVazquez Gomez, R.
dc.contributor.authorMarin Benito, Carla
dc.date.accessioned2022-05-10T14:47:53Z
dc.date.available2022-05-10T14:47:53Z
dc.date.issued2021
dc.date.updated2022-05-10T14:47:53Z
dc.description.abstractThe first full angular analysis of the B0 → D∗−D∗+ s decay is performed using 6 fb−1 of pp collision data collected with the LHCb experiment at a centre-of-mass energy of 13 TeV. The D∗+ s → D+ s γ and D∗− → D 0 π − vector meson decays are used with the subsequent D+ s → K+K−π + and D 0 → K+π − decays. All helicity amplitudes and phases are measured, and the longitudinal polarisation fraction is determined to be fL = 0.578±0.010±0.011 with world-best precision, where the first uncertainty is statistical and the second is systematic. The pattern of helicity amplitude magnitudes is found to align with expectations from quark-helicity conservation in B decays. The ratio of branching fractions [B(B0 → D∗−D∗+ s ) × B(D∗+ s → D+ s γ)]/B(B0 → D∗−D+ s ) is measured to be 2.045 ± 0.022 ± 0.071 with world-best precision. In addition, the first observation of the Cabibbo-suppressed Bs → D∗−D+ s decay is made with a significance of seven standard deviations. The branching fraction ratio B(Bs → D∗−D+ s )/B(B0 → D∗−D+ s ) is measured to be 0.049 ± 0.006 ± 0.003 ± 0.002, where the third uncertainty is due to limited knowledge of the ratio of fragmentation fractions.
dc.format.extent30 p.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec721071
dc.identifier.issn1126-6708
dc.identifier.urihttps://hdl.handle.net/2445/185482
dc.language.isoeng
dc.publisherSpringer Verlag
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.1007/JHEP06(2021)177
dc.relation.ispartofJournal of High Energy Physics, 2021, vol. 2021, p. 1-30
dc.relation.urihttps://doi.org/10.1007/JHEP06(2021)177
dc.rightscc-by (c) LHCb Collaboration et al., 2021
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.sourceArticles publicats en revistes (Física Quàntica i Astrofísica)
dc.subject.classificationHadrons
dc.subject.classificationGran Col·lisionador d'Hadrons
dc.subject.classificationFísica de partícules
dc.subject.classificationExperiments
dc.subject.otherHadrons
dc.subject.otherLarge Hadron Collider (France and Switzerland)
dc.subject.otherParticle physics
dc.subject.otherExperiments
dc.titleAngular analysis of B0→D∗−D∗+s with D∗+s→D+sγ decays
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/publishedVersion

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