D-meson semileptonic decays to pseudoscalars from four-flavor lattice QCD
Abstract
We present lattice-QCD calculations of the hadronic form factors for the semileptonic decays , , and . Our calculation uses the highly improved staggered quark (HISQ) action for all valence and sea quarks and includes MILC ensembles with lattice spacings ranging from fm down to fm. At most lattice spacings, an ensemble with physical-mass light quarks is included. The HISQ action allows all the quarks to be treated with the same relativistic light-quark action, allowing for nonperturbative renormalization using partial conservation of the vector current. We combine our results with experimental measurements of the differential decay rates to determine and This result for is the most precise to date, with a lattice-QCD error that is, for the first time for the semileptonic extraction, at the same level as the experimental error. Using recent measurements from BES III, we also give the first-ever determination of from . Our results also furnish new Standard Model calculations of the lepton flavor universality ratios , , and , which are consistent within with experimental measurements. Our extractions of and , when combined with a value for , provide the most precise test of second-row CKM unitarity, finding agreement with unitarity at the level of one standard deviation.
Keywords
Cite
@article{arxiv.2212.12648,
title = {D-meson semileptonic decays to pseudoscalars from four-flavor lattice QCD},
author = {Alexei Bazavov and Carleton DeTar and Aida X. El-Khadra and Elvira Gámiz and Zechariah Gelzer and Steven Gottlieb and William I. Jay and Hwancheol Jeong and Andreas S. Kronfeld and Ruizi Li and Andrew T. Lytle and Paul B. Mackenzie and Ethan T. Neil and Thomas Primer and James N. Simone and Robert L. Sugar and Doug Toussaint and Ruth S. Van de Water and Alejandro Vaquero},
journal= {arXiv preprint arXiv:2212.12648},
year = {2023}
}
Comments
92 pages, V2 matches version accepted for publication in PRD. Expanded supplementary material for reconstructing our final results. An implementation of nonlinear shrinkage is also included