Chiral dynamics and S-wave contributions in $\bar B^0/D^0 \to \pi^{\pm}\eta\ l^{\mp} \nu$ decays

TL;DR

This paper investigates semi-leptonic B and D meson decays involving the a0(980) scalar resonance, using light-cone sum rules and unitarized chiral perturbation theory to model final-state interactions, providing predictions consistent with experimental data.

Contribution

It introduces a novel analysis of these decays incorporating finite-width effects via scalar form factors derived from unitarized chiral perturbation theory.

Findings

D meson decay branching fraction matches BESIII measurements.

Predicted B meson decay branching fraction can be tested in future experiments.

Method effectively accounts for final-state interactions in semi-leptonic decays.

Abstract

In this work, we analyze the semi-leptonic decays $\bar B^0/D^0 \to (a_0(980)^{\pm}\to\pi^{\pm}\eta) l^{\mp} \nu$ within light-cone sum rules. The two and three-body light-cone distribution amplitudes (LCDAs) of the $B$ meson and the only available two-body LCDA of the $D$ meson are used. To include the finite-width effect of the $a_0(980)$, we use a scalar form factor to describe the final-state interaction between the $\pi\eta$ mesons, which was previously calculated within unitarized Chiral Perturbation Theory. The result for the decay branching fraction of the $D^0$ decay is in good agreement with that measured by the BESIII Collaboration, while the branching fraction of the $\bar B^0$ decay can be tested in future experiments.