Please use this identifier to cite or link to this item: http://hdl.handle.net/2445/185482
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dc.contributor.authorLHCb Collaboration-
dc.contributor.authorAlfonso Albero, Alejandro-
dc.contributor.authorGarcia Moreno, P.-
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.identifier.issn1126-6708-
dc.identifier.urihttp://hdl.handle.net/2445/185482-
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.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.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-
dc.identifier.idgrec721071-
dc.date.updated2022-05-10T14:47:53Z-
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess-
Appears in Collections:Articles publicats en revistes (Física Quàntica i Astrofísica)

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