QCD factorization of the four-lepton decay $B^-\rightarrow \ell \bar{\nu}_\ell \ell^{(\prime)} \bar{\ell}^{(\prime)}$

TL;DR

This paper calculates the decay amplitude for the rare four-lepton $B^-$ decay using factorization, providing predictions for branching fractions and exploring sensitivity to the $B$ meson distribution amplitude, relevant for experimental searches.

Contribution

It introduces a factorization-based calculation of the $B^- o ext{4 leptons}$ decay amplitude, including form factors and their dependence on invariant masses, with predictions for branching fractions and sensitivity analysis.

Findings

Branching fractions are a few times 10^{-8} up to 1 GeV^2 in $q^2$.

Decay rate is highly sensitive to the inverse moment $ ext{λ}_B$ at small $q^2$.

The decay rate drops rapidly with increasing $q^2$.

Abstract

Motivated by the first search for the rare charged-current $B$ decay to four leptons, $\ell \bar{\nu}_\ell \ell^{(\prime)} \bar{\ell}^{(\prime)}$, we calculate the decay amplitude with factorization methods. We obtain the $B\to \gamma^*$ form factors, which depend on the invariant masses of the two lepton pairs, at leading power in an expansion in $\Lambda_{\rm QCD}/m_b$ to next-to-leading order in $\alpha_s$, and at $\mathcal{O}(\alpha_s^0)$ at next-to-leading power. Our calculations predict branching fractions of a few times $10^{-8}$ in the $\ell^{(\prime)} \bar{\ell}^{(\prime)}$ mass-squared bin up to $q^2=1~\text{GeV}^2$ with $n_+q>3~$GeV. The branching fraction rapidly drops with increasing $q^2$. An important further motivation for this investigation has been to explore the sensitivity of the decay rate to the inverse moment $\lambda_B$ of the leading-twist $B$ meson light-cone distribution amplitude. We find that in the small-$q^2$ bin, the sensitivity to $\lambda_B$ is almost comparable to $B^- \rightarrow \ell^- \bar{\nu}_\ell\gamma$ when $\lambda_B$ is small, but with an added uncertainty from the light-meson intermediate resonance contribution. The sensitivity degrades with larger $q^2$.