Structure-dependent QED in $B^{-}\to {\ell }^{-}\bar{\hat{I}}½({\hat{I}}^3)$

Abstract

Based on explicitly gauge invariant interpolating operators we compute complete next-leading order QED-corrections for leptonic decays. These are sizeable since the helicity-suppression in V-A interactions allows for structure-dependent collinear logs. We have explicitly checked that these logs are absent for helicity-unsuppressed Yukawa-type transitions. Based on $B\to {\hat{I}}^3$ form factors we present the rates for $B^{-}\to (\hat{I}{¼}^{-},\ddot{I}{„}^{-})\bar{\hat{I}}½({\hat{I}}^3)$ in differential and integrated form as a function of the photon energy cut-off $E_γ^{\text{cut}}$. The effect of the virtual structure-dependent corrections are approximately $+5\%$ and $+3\%$ for the $\hat{I}¼$- and $\ddot{I}„$-channel respectively. The structure dependence of the real radiation exceeds that of the virtual one for $E_γ^{\text{cut}}|_μ > 0.18(3)$ GeV and is subdominant for the tau channel even when fully inclusive.

31 pp, 12 figs, ancillary Mathematica notebook explaining how to combine real and virtual contributions