Semileptonic form factors for B→ D∗ℓν at nonzero recoil from 2 + 1 -flavor lattice QCD: Fermilab Lattice and MILC Collaborations
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Author
Bazavov, A.DeTar, C.E.
Du, D.
El-Khadra, A.X.
Gámiz, E.
Gelzer, Z.
Gottlieb, S.
Heller, U.M.
Kronfeld, A.S.
Laiho, J.
Mackenzie, P.B.
Simone, J.N.
Sugar, R.
Toussaint, D.
Van de Water, R.S.
Vaquero, A.
Affiliation
Department of Physics, University of ArizonaIssue Date
2022-12-16
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Institute for IonicsCitation
Bazavov, A., DeTar, C. E., Du, D., El-Khadra, A. X., Gámiz, E., Gelzer, Z., Gottlieb, S., Heller, U. M., Kronfeld, A. S., Laiho, J., Mackenzie, P. B., Simone, J. N., Sugar, R., Toussaint, D., Van de Water, R. S., & Vaquero, A. (2022). Semileptonic form factors for B→ D∗ℓν at nonzero recoil from 2 + 1 -flavor lattice QCD: Fermilab Lattice and MILC Collaborations. European Physical Journal C, 82(12).Journal
European Physical Journal CRights
© The Author(s) 2022. This article is licensed under a Creative Commons Attribution 4.0 International License, (http://creativecommons.org/licenses/by/4.0/).Collection Information
This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.Abstract
We present the first unquenched lattice-QCD calculation of the form factors for the decay B→ D∗ℓν at nonzero recoil. Our analysis includes 15 MILC ensembles with Nf= 2 + 1 flavors of asqtad sea quarks, with a strange quark mass close to its physical mass. The lattice spacings range from a≈ 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 | Vcb|. We obtain | Vcb| = (38.40 ± 0. 68 th± 0. 34 exp± 0. 18 EM) × 10 - 3. The first error is theoretical, the second comes from experiment and the last one includes electromagnetic and electroweak uncertainties, with an overall χ2/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. © 2022, The Author(s).Note
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1434-6044Version
Final published versionae974a485f413a2113503eed53cd6c53
10.1140/epjc/s10052-022-10984-9
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Except where otherwise noted, this item's license is described as © The Author(s) 2022. This article is licensed under a Creative Commons Attribution 4.0 International License, (http://creativecommons.org/licenses/by/4.0/).

