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dc.contributor.authorBazavov, A.
dc.contributor.authorGámiz Sánchez, María Elvira 
dc.contributor.authorFermilab Lattice Collaboration
dc.contributor.authorMILC Collaboration
dc.date.accessioned2023-01-24T09:11:08Z
dc.date.available2023-01-24T09:11:08Z
dc.date.issued2022-12-16
dc.identifier.citationBazavov, A... [et al.]. Semileptonic form factors for B\rightarrow D^*\ell \nu at nonzero recoil from 2+1-flavor lattice QCD. Eur. Phys. J. C 82, 1141 (2022). [https://doi.org/10.1140/epjc/s10052-022-10984-9]es_ES
dc.identifier.urihttps://hdl.handle.net/10481/79292
dc.description.abstractWe present the first unquenched lattice-QCD calculation of the form factors for the decay B -> D*t nu at nonzero recoil. Our analysis includes 15 MILC ensembles with N-f = 2 + 1 flavors of asqtad sea quarks, with a strange quark mass close to its physical mass. The lattice spacings range from a asymptotic to 0.15 fm down to 0.045 fm, while the ratio between the light-and the strange-quark masses ranges from 0.05 to 0.4. The valence b and c quarks are treated using the Wilson-clover action with the Fermilab interpretation, whereas the light sector employs asqtad staggered fermions. We extrapolate our results to the physical point in the continuum limit using rooted staggered heavy-light meson chiral perturbation theory. Then we apply a model independent parametrization to extend the form factors to the full kinematic range. With this parametrization we perform a joint lattice-QCD/experiment fit using several experimental datasets to determine the CKM matrix element |V-cb|. We obtain |V-cb| = (38.40 +/- 0.68(th) +/- 0.34(exp) +/- 0.18(EM)) x 10(-3). The first error is theoretical, the second comes from experiment and the last one includes electromagnetic and electroweak uncertainties, with an overall chi(2)/dof = 126/84, which illustrates the tensions between the experimental data sets, and between theory and experiment. This result is in agreement with previous exclusive determinations, but the tension with the inclusive determination remains. Finally, we integrate the differential decay rate obtained solely from lattice data to predict R(D*) = 0.265 +/- 0.013, which confirms the current tension between theory and experiment.es_ES
dc.description.sponsorshipUnited States Department of Energy (DOE)es_ES
dc.description.sponsorshipNational Science Foundation's Teragrid/XSEDE Programes_ES
dc.description.sponsorshipUnited States Department of Energy (DOE) DE-FG02-13ER41976 DE-SC0009998 DE-SC0010120 DE-SC0015655es_ES
dc.description.sponsorshipNational Science Foundation (NSF) PHY17-19626 PHY14-17805 SRA (Spain) P18-FR-4314es_ES
dc.description.sponsorshipConsejeria de Economia, Innovacion, Ciencia y Empleo, Junta de Andalucia (Spain) P18-FR-4314 A-FQM-467-UGR18es_ES
dc.description.sponsorshipFermilab Distinguished Scholars Programes_ES
dc.language.isoenges_ES
dc.publisherSpringeres_ES
dc.rightsAtribución 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.titleSemileptonic form factors for B -> D*lv at nonzero recoil from 2+1-flavor lattice QCDes_ES
dc.typejournal articlees_ES
dc.rights.accessRightsopen accesses_ES
dc.identifier.doi10.1140/epjc/s10052-022-10984-9
dc.type.hasVersionVoRes_ES


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