Abstract

We determine the normalisation of scalar and pseudoscalar current operators made from non-relativistic $b$ quarks and Highly Improved Staggered light quarks in lattice Quantum Chromodynamics (QCD) through $\mathcal{O}(\alpha_s)$ and $\Lambda_{\text{QCD}}/m_b$. We use matrix elements of these operators to extract $B$ meson decay constants and form factors, then compare to those obtained using the standard vector and axial-vector operators. This provides a test of systematic errors in the lattice QCD determination of the $B$ meson decay constants and form factors. We provide a new value for the $B$ and $B_s$ meson decay constants from lattice QCD calculations on ensembles that include $u$, $d$, $s$ and $c$ quarks in the sea and those which have the $u/d$ quark mass going down to its physical value. Our results are $f_B=0.196(6)$ GeV, $f_{B_s}=0.236(7)$ GeV and $f_{B_s}/f_B =1.207(7)$, agreeing well with earlier results using the temporal axial current. By combining with these previous results, we provide updated values of $f_B=0.190(4)$ GeV, $f_{B_s}=0.229(5)$ GeV and $f_{B_s}/f_B = 1.206(5)$.

Highlights

  • Hadronic weak decay matrix elements containing b quarks that are calculated in lattice quantum chromodynamics (QCD) are critical to the flavor physics program of overdetermining the Cabibbo-Kobayashi-Maskawa (CKM) matrix in order to find signs of new physics

  • They include multiple values of the lattice spacing and multiple values of the u=d sea quark mass varying from one-fifth of the s quark mass down to the physical value

  • On these gluon field configurations the B and Bs decay constants were calculated in [9] using a radiatively improved NonRelativistic Quantum Chromodynamics (NRQCD) action for the b quark [22,26], the highly improved staggered quarks (HISQ) action for the lighter quark, and an NRQCD-HISQ temporal axial current matched to continuum QCD following the process described in Sec

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Summary

Introduction

Hadronic weak decay matrix elements containing b quarks that are calculated in lattice quantum chromodynamics (QCD) are critical to the flavor physics program of overdetermining the Cabibbo-Kobayashi-Maskawa (CKM) matrix in order to find signs of new physics. The accuracy of the lattice QCD results often limits the accuracy with which the CKM matrix elements can be determined and with which the associated unitarity tests can be performed [1]. It is important both to improve and to test the accuracy of the lattice QCD results. This includes determining the lattice QCD values using a variety of different

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