Comprehensive analysis of local and nonlocal amplitudes in the B0 → K∗0µ +µ − decay

dc.contributor.authorComerma Montells, Albert
dc.contributor.authorGarcia Moreno, Paula
dc.contributor.authorGarrido Beltrán, Lluís
dc.contributor.authorGioventù, Alessandra
dc.contributor.authorGironella Gironell, Pere
dc.contributor.authorGomez Fernandez, Sergio
dc.contributor.authorGraugés Pous, Eugeni
dc.contributor.authorLobo Salvia, Aniol
dc.contributor.authorLópez Huertas, Albert
dc.contributor.authorManera Escalero, Rafel
dc.contributor.authorMarin Benito, Carla
dc.contributor.authorMauricio Ferre, Joan
dc.contributor.authorCalefice, Lukas
dc.contributor.authorVazquez Gomez, Ricardo
dc.contributor.authorLHCb Collaboration
dc.date.accessioned2025-06-27T13:21:37Z
dc.date.available2025-06-27T13:21:37Z
dc.date.issued2024
dc.date.updated2025-06-27T13:21:37Z
dc.description.abstractA comprehensive study of the local and nonlocal amplitudes contributing to the decay B0 → K∗0 (→ K+π −)µ +µ − is performed by analysing the phase-space distribution of the decay products. The analysis is based on pp collision data corresponding to an integrated luminosity of 8.4 fb−1 collected by the LHCb experiment. This measurement employs for the frst time a model of both one-particle and two-particle nonlocal amplitudes, and utilises the complete dimuon mass spectrum without any veto regions around the narrow charmonium resonances. In this way it is possible to explicitly isolate the local and nonlocal contributions and capture the interference between them. The results show that interference with nonlocal contributions, although larger than predicted, only has a minor impact on the Wilson Coefcients determined from the ft to the data. For the local contributions, the Wilson Coefcient C9, responsible for vector dimuon currents, exhibits a 2.1σ deviation from the Standard Model expectation. The Wilson Coefcients C10, C ′ 9 and C ′ 10 are all in better agreement than C9 with the Standard Model and the global signifcance is at the level of 1.5σ. The model used also accounts for nonlocal contributions from B0 → K∗0 τ +τ − → µ +µ − rescattering, resulting in the frst direct measurement of the bsτ τ vector efective-coupling C9τ .
dc.format.extent60 p.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec756463
dc.identifier.issn1126-6708
dc.identifier.urihttps://hdl.handle.net/2445/221843
dc.language.isoeng
dc.publisherSpringer Verlag
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.1007/JHEP09(2024)026
dc.relation.ispartofJournal of High Energy Physics, 2024, vol. 2024, num.26
dc.relation.urihttps://doi.org/10.1007/JHEP09(2024)026
dc.rightscc-by (c) Aaij, R. et al., 2024
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/
dc.sourceArticles publicats en revistes (Física Quàntica i Astrofísica)
dc.subject.classificationModel estàndard (Física nuclear)
dc.subject.classificationFísica de partícules
dc.subject.classificationHadrons
dc.subject.otherStandard model (Nuclear physics)
dc.subject.otherParticle physics
dc.subject.otherHadrons
dc.titleComprehensive analysis of local and nonlocal amplitudes in the B0 → K∗0µ +µ − decay
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/publishedVersion

Fitxers

Paquet original

Mostrant 1 - 1 de 1
Carregant...
Miniatura
Nom:
886281.pdf
Mida:
7.59 MB
Format:
Adobe Portable Document Format