The B*Bpi coupling using relativistic heavy quarks
J.M. Flynn, P. Fritzsch, T. Kawanai, C. Lehner, B. Samways, C.T., Sachrajda, R.S. Van de Water, O. Witzel (for the RBC/UKQCD Collaboration)

TL;DR
This paper presents a lattice QCD calculation of the B*Bpi coupling directly at the physical b-quark mass, providing a precise determination of a key low-energy constant in heavy meson chiral perturbation theory.
Contribution
It is the first direct lattice QCD calculation of the B*Bpi coupling at the physical b-quark mass, controlling systematic uncertainties and using multiple lattice spacings and pion masses.
Findings
Final result for g_b = 0.56(3)stat(7)sys
Achieved good statistical precision and systematic control
Performed at physical b-quark mass with multiple lattice spacings
Abstract
We report on a calculation of the B*Bpi coupling in lattice QCD. The strong matrix element for a B* to Bpi transition is directly related to the leading order low-energy constant in heavy meson chiral perturbation theory (HMChPT) for B mesons. We carry out our calculation directly at the b-quark mass using a non-perturbatively tuned clover action that controls discretization effects of order pa and (ma)^n for all n. Our analysis is performed on RBC/UKQCD gauge configurations using domain-wall fermions and the Iwasaki gauge action at two lattice spacings of ainverse = 1.729(25) GeV, ainverse = 2.281(28) GeV, and unitary pion masses down to 290 MeV. We achieve good statistical precision and control all systematic uncertainties, giving a final result for the HMChPT coupling g_b = 0.56(3)stat(7)sys in the continuum and at the physical light-quark masses. This is the first calculation…
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