QCD calculations of $B \to \pi, K$ form factors with higher-twist corrections

TL;DR

This paper refines QCD calculations of $B o \pi,K$ form factors by including higher-twist corrections and strange-quark mass effects, improving theoretical precision for semileptonic and rare B decays.

Contribution

It introduces a comprehensive higher-twist correction framework for $B$-meson LCDAs and applies it to improve form factor calculations and phenomenological predictions.

Findings

Higher-twist corrections significantly affect form factor estimates.

Strange-quark mass effects are leading-power contributions in the heavy quark expansion.

Enhanced predictions for $B o \pi,K$ decay observables and CKM matrix element $|V_{ub}|$.

Abstract

We update QCD calculations of $B \to \pi, K$ form factors at large hadronic recoil by including the subleading-power corrections from the higher-twist $B$-meson light-cone distribution amplitudes (LCDAs) up to the twist-six accuracy and the strange-quark mass effects at leading-power in $\Lambda/m_b$ from the twist-two $B$-meson LCDA $\phi_B^{+}(\omega, \mu)$. The higher-twist corrections from both the two-particle and three-particle $B$-meson LCDAs are computed from the light-cone QCD sum rules (LCSR) at tree level. In particular, we construct the local duality model for the twist-five and -six $B$-meson LCDAs, in agreement with the corresponding asymptotic behaviours at small quark and gluon momenta, employing the QCD sum rules in heavy quark effective theory at leading order in $\alpha_s$. The strange quark mass effects in semileptonic $B \to K$ form factors yield the leading-power contribution in the heavy quark expansion, consistent with the power-counting analysis in soft-collinear effective theory, and they are also computed from the LCSR approach due to the appearance of the rapidity singularities. We further explore the phenomenological aspects of the semileptonic $B \to \pi \ell \nu$ decays and the rare exclusive processes $B \to K \nu \nu$, including the determination of the CKM matrix element $|V_{ub}|$, the normalized differential $q^2$ distributions and precision observables defined by the ratios of branching fractions for the above-mentioned two channels in the same intervals of $q^2$.