Abstract

We calculate the leptonic decay constants of heavy-light pseudoscalar mesons with charm and bottom quarks in lattice quantum chromodynamics on four-flavor QCD gauge-field configurations with dynamical $u$, $d$, $s$, and $c$ quarks. We analyze over twenty isospin-symmetric ensembles with six lattice spacings down to $a\approx 0.03$~fm and several values of the light-quark mass down to the physical value $\frac{1}{2}(m_u+m_d)$. We employ the highly-improved staggered-quark (HISQ) action for the sea and valence quarks; on the finest lattice spacings, discretization errors are sufficiently small that we can calculate the $B$-meson decay constants with the HISQ action for the first time directly at the physical $b$-quark mass. We obtain the most precise determinations to-date of the $D$- and $B$-meson decay constants and their ratios, $f_{D^+} = 212.7(0.6)$~MeV, $f_{D_s} = 249.9(0.4)$~MeV, $f_{D_s}/f_{D^+} = 1.1749(16)$, $f_{B^+} = 189.4 (1.4)$~MeV, $f_{B_s} = 230.7(1.3)$~MeV, $f_{B_s}/f_{B^+} = 1.2180(47)$, where the errors include statistical and all systematic uncertainties. Our results for the $B$-meson decay constants are three times more precise than the previous best lattice-QCD calculations, and bring the QCD errors in the Standard-Model predictions for the rare leptonic decays $\overline{\mathcal{B}}(B_s \to \mu^+\mu^-) = 3.64(11) \times 10^{-9}$, $\overline{\mathcal{B}}(B^0 \to \mu^+\mu^-) = 1.00(3) \times 10^{-10}$, and $\overline{\mathcal{B}}(B^0 \to \mu^+\mu^-)/\overline{\mathcal{B}}(B_s \to \mu^+\mu^-) = 0.0273(9)$ to well below other sources of uncertainty. As a byproduct of our analysis, we also update our previously published results for the light-quark-mass ratios and the scale-setting quantities $f_{p4s}$, $M_{p4s}$, and $R_{p4s}$. We obtain the most precise lattice-QCD determination to date of the ratio $f_{K^+}/f_{\pi^+} = 1.1950(^{+16}_{-23})$~MeV.

Highlights

  • Leptonic decays of B and D mesons are important probes of heavy-to-light quark flavor-changing interactions

  • The charged-current decays Hþ → lþνl (H 1⁄4 Dþ; Ds; Bþ; l 1⁄4 e, μ, τ) proceed at tree level in the standard model via the axial-vector current Aμ ≡ Qγ5γμq, where Q is the heavy charm or bottom quark and q is the light quark in the pseudoscalar meson

  • Because the decays H0 → lþl− (H 1⁄4 D0; B0; Bs) proceed via a flavor-changing-neutral-current interaction, and are forbidden at tree level in the standard model, these processes may be especially sensitive to contributions of new heavy particles. Both the standard model and new-physics predictions for the rare-decay branching ratios depend upon the decay constants fH0

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Summary

INTRODUCTION

Leptonic decays of B and D mesons are important probes of heavy-to-light quark flavor-changing interactions. Our previous calculation [23] of the DðsÞ-meson decay constants employed physical-mass light and charm quarks and gauge-field configurations with lattice spacings down to a ≈ 0.06 fm; the dominant contribution to the errors on fD and fDs came from the continuum extrapolation. HPQCD’s calculation of fBs with the HISQ action for the b quark employed five three-flavor ensembles of gauge-field configurations from the MILC Collaboration [30,31,32] with lattice spacings as fine as a ≈ 0.045 fm, enabling them to simulate with heavy-quark masses close to the physical bottom-quark mass. Appendix C provides the correlation and covariance matrices between our B- and D-meson decay constant results

SIMULATION PARAMETERS AND METHODS
Simulation parameters
RHMC and RHMD algorithms
TWO-POINT CORRELATOR FITS
LATTICE SPACING AND QUARK-MASS TUNING
EFFECTIVE-FIELD-THEORY ANALYSIS
Effective-field-theory fit function for heavy-light decay constants
Summary formula
Setting the lattice scale for the EFT analysis
Effective-field-theory fit to heavy-light decay constants
SYSTEMATIC ERROR BUDGETS
B- and D-meson decay constants
CKM matrix elements
VIII. SUMMARY AND OUTLOOK
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