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

R. AaijNikhef National Institute for Subatomic PhysicsA. S. W. AbdelmottelebUniversity of WarwickC. Abellán BetetaUniversität ZürichT. AckernleyUniversity of LiverpoolA. A. AdefisoyeSyracuse UniversityB. AdevaUniversidade de Santiago de CompostelaM. AdinolfiUniversity of BristolP. AdlarsonUppsala UniversityC. AgapopoulouUniversité Paris-Saclay, CNRS/IN2P3, IJCLabC. A. AidalaUniversity of MichiganZ. AjaltouniUniversité Clermont Auvergne, CNRS/IN2P3, LPCS. AkarUniversity of CincinnatiK. Carvalho AkibaNikhef National Institute for Subatomic PhysicsP. AlbicoccoINFN Laboratori Nazionali di FrascatiJ. AlbrechtTechnische Universität DortmundF. AlessioEuropean Organization for Nuclear Research (CERN)M. AlexanderUniversity of GlasgowZakariya AlioucheUniversity of ManchesterP. Álvarez CartelleUniversity of CambridgeR. AmalricLPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3S. AmatoUniversidade Federal do Rio de Janeiro (UFRJ)S. AmatoUniversity of BristolY. AmhisEuropean Organization for Nuclear Research (CERN)L. AnPeking UniversityL. AnINFN Sezione di FirenzeM. AnderssonUniversität ZürichA. AndreianovP. AndreolaUniversität ZürichM. AndreottiINFN Sezione di FerraraD. AndreouSyracuse UniversityAlessia AnelliINFN Sezione di Milano-BicoccaD. AoUniversity of Chinese Academy of SciencesF. ArchilliINFN Sezione di Roma Tor VergataMatteo ArgentonINFN Sezione di FerraraS. Arguedas CuendisConsejo Nacional de Rectores (CONARE)A. ArtamonovM. ArtusoSyracuse UniversityE. AslanidesAix Marseille Univ, CNRS/IN2P3, CPPMR. Ataide Da SilvaEcole Polytechnique Fédérale de Lausanne (EPFL)M. AtzeniMassachusetts Institute of TechnologyB. AudurierInstitut Polytechnique de ParisD. BacherUniversity of OxfordI. Bachiller PereaUniversité Savoie Mont Blanc, CNRS, IN2P3-LAPPS. BachmannRuprecht-Karls-Universität HeidelbergM. BachmayerEcole Polytechnique Fédérale de Lausanne (EPFL)J. J. BackUniversity of WarwickP. Baladrón RodríguezUniversidade de Santiago de CompostelaV. BalaguraInstitut Polytechnique de ParisW. BaldiniINFN Sezione di FerraraH. BaoUniversity of Chinese Academy of SciencesJ. Baptista de Souza LeiteUniversity of LiverpoolM. BarbettiINFN Sezione di FirenzeI. R. BarbosaPontifícia Universidade Católica do Rio de Janeiro (PUC-Rio)R. J. BarlowUniversity of ManchesterMikhail BarnyakovINFN Sezione di BolognaS. BarsukUniversité Paris-Saclay, CNRS/IN2P3, IJCLabW. BarterUniversity of EdinburghM. BartoliniUniversity of CambridgeJustin BartzSyracuse UniversityJ. M. BaselsRWTH Aachen UniversityG. BassiINFN Sezione di PisaB. BatsukhA. BayEcole Polytechnique Fédérale de Lausanne (EPFL)A. BeckUniversity of WarwickM. BeckerTechnische Universität DortmundF. BedeschiINFN Sezione di PisaI. BediagaCentro Brasileiro de Pesquisas Físicas (CBPF)A. BeiterUniversidade de Santiago de CompostelaV. BelléeUniversität ZürichK. BelousI. BelovINFN Sezione di GenovaI. BelyaevINFN Sezione di Roma La SapienzaG. BenaneAix Marseille Univ, CNRS/IN2P3, CPPMG. BencivenniINFN Laboratori Nazionali di FrascatiE. Ben-HaimLPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3A. BerezhnoyR. BernetUniversität ZürichH. C. BernsteinUniversitat Ramon LlullA. BertolinINFN Sezione di PadovaC. BetancourtUniversität ZürichF. BettiUniversity of EdinburghJ. BexUniversity of CambridgeIa. BezshyikoUniversität ZürichJ. BhomHenryk Niewodniczanski Institute of Nuclear Physics Polish Academy of SciencesM. S. BiekerTechnische Universität DortmundN. V. BiesuzINFN Sezione di FerraraP. BilloirLPNHE, Sorbonne Université, Paris Diderot Sorbonne Paris Cité, CNRS/IN2P3A. BiolchiniNikhef National Institute for Subatomic PhysicsM. BirchImperial College LondonF. C. R. BishopUniversité Savoie Mont Blanc, CNRS, IN2P3-LAPPA. BitadzeUniversity of ManchesterA. BizzetiT. BlakeUniversity of WarwickF. BlancEcole Polytechnique Fédérale de Lausanne (EPFL)J. E. BlankTechnische Universität DortmundS. BluskSyracuse UniversityVladimir BocharnikovJ. A. BoelhauveTechnische Universität DortmundO. Boente GarcíaInstitut Polytechnique de Paris
2024en
ABI

Abstract

A bstract A comprehensive study of the local and nonlocal amplitudes contributing to the decay B 0 → 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 first 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 Coefficients determined from the fit to the data. For the local contributions, the Wilson Coefficient $$ {\mathcal{C}}_9 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>C</mml:mi> <mml:mn>9</mml:mn> </mml:msub> </mml:math> , responsible for vector dimuon currents, exhibits a 2.1 σ deviation from the Standard Model expectation. The Wilson Coefficients $$ {\mathcal{C}}_{10} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>C</mml:mi> <mml:mn>10</mml:mn> </mml:msub> </mml:math> , $$ {\mathcal{C}}_9^{\prime } $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>C</mml:mi> <mml:mn>9</mml:mn> <mml:mo>′</mml:mo> </mml:msubsup> </mml:math> and $$ {\mathcal{C}}_{10}^{\prime } $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>C</mml:mi> <mml:mn>10</mml:mn> <mml:mo>′</mml:mo> </mml:msubsup> </mml:math> are all in better agreement than $$ {\mathcal{C}}_9 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>C</mml:mi> <mml:mn>9</mml:mn> </mml:msub> </mml:math> with the Standard Model and the global significance is at the level of 1.5 σ . The model used also accounts for nonlocal contributions from B 0 → K *0 [ τ + τ − → μ + μ − ] rescattering, resulting in the first direct measurement of the bsττ vector effective-coupling $$ {\mathcal{C}}_{9\tau } $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>C</mml:mi> <mml:mrow> <mml:mn>9</mml:mn> <mml:mi>τ</mml:mi> </mml:mrow> </mml:msub> </mml:math> .

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