Extracting $B_s\to D_s^*\ell u_\ell$ form factors

Semileptonic $B_{(s)}$ decays are of great phenomenological interest because they allow to determine e.g. CKM matrix elements or test lepton flavor universality. Taking advantage of already existing lattice data, we demonstrate the analysis steps to extract the four form factors describing exclusive semileptonic $B_s\to D_s^*\ell\nu_\ell$ decays using the narrow width approximation. Our data are based on RBC/UKQCD's set of 2+1 flavor gauge field ensembles with Shamir domain-wall fermion and Iwasaki gauge field action featuring inverse lattice spacings of $a^{-1}=$1.785, 2.383, and 2.785 GeV as well as pion masses between 268 and 433 MeV. Light, strange and charm quarks are simulated using domain-wall fermions, whereas bottom quarks are generated with the relativistic heavy quark (RHQ) action.

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Publication Details

Published
2026-04-14
DOI
https://doi.org/10.22323/1.518.0237
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
0.00

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article

Extracting $B_s\to D_s^*\ell u_\ell$ form factors

Anastasia Boushmelev, Matthew Black, Oliver Witzel
Particle physics theoretical and experimental studies
article

Extracting $B_s\to D_s^*\ell u_\ell$ form factors

Anastasia Boushmelev, Matthew Black, Oliver Witzel
article en

Abstract

Semileptonic $B_{(s)}$ decays are of great phenomenological interest because they allow to determine e.g. CKM matrix elements or test lepton flavor universality. Taking advantage of already existing lattice data, we demonstrate the analysis steps to extract the four form factors describing exclusive semileptonic $B_s\to D_s^*\ell\nu_\ell$ decays using the narrow width approximation. Our data are based on RBC/UKQCD's set of 2+1 flavor gauge field ensembles with Shamir domain-wall fermion and Iwasaki gauge field action featuring inverse lattice spacings of $a^{-1}=$1.785, 2.383, and 2.785 GeV as well as pion masses between 268 and 433 MeV. Light, strange and charm quarks are simulated using domain-wall fermions, whereas bottom quarks are generated with the relativistic heavy quark (RHQ) action.

U.S. Department of Energy, Universität Siegen, Deutsche Forschungsgemeinschaft, Office of Science, Science and Technology Facilities Council, High Energy Physics, Fermilab, Brookhaven National Laboratory
Openalex Percentile: Top 11%
Particle physics theoretical and experimental studies
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