Factorization of radiative leptonic D-meson decay with sub-leading power corrections

TL;DR

This paper calculates sub-leading power corrections to the radiative leptonic D-meson decay, providing analytic expressions and estimating uncertainties, revealing significant effects on form factors and branching fractions.

Contribution

It presents the first analytic expressions for next-to-leading power contributions and evaluates their impact on decay form factors and branching ratios.

Findings

Sub-leading power contributions are significant at specified parameters.

Next-to-leading power corrections can exceed 100% of leading power effects.

Predicted branching fractions are approximately 1.9 and 2.3 times 10^{-5}.

Abstract

In this work, we calculate the sub-leading power contributions to the radiative leptonic $D\to\gamma \,\ell \,\nu$ decay. For the first time, we provide the analytic expressions of next-to-leading power contributions and the error estimation associated with the power expansion of ${\cal O}(\Lambda_{\rm QCD}/m_c)$. In our calculation, we adopt two different models of the $D$-meson distribution amplitudes $\phi_{D,\rm I}^+$ and $\phi_{D,\rm II}^+$. Within the framework of the QCD factorization as well as the dispersion relation, we evaluate the soft contribution up to the next-to-leading logarithmic accuracy, and the higher-twist contribution from the two-particle and three-particle distribution amplitudes is also considered. Finally, we find that all the sub-leading power contributions are significant at $\lambda_D(\mu_0)=354\,\rm MeV$, and the next-to-leading power contributions will lead to $143\%$ in $\phi_{D,\rm I}^+$ and $120\%$ in $\phi_{D,\rm II}^+$ corrections to leading power vector form factors with $E_{\gamma}=0.5\,\rm GeV$. As the corrections from the higher-twist and local sub-leading power contributions will be enhanced with the growing of the inverse moment, it is difficult to extract an appropriate inverse moment of the $D$-meson distribution amplitude. The predicted branching fractions are $(1.88_{-0.29}^{+0.36})\times10^{-5}$ for $\phi_{D,\rm I}^+$ and $(2.31_{-0.54}^{+0.65})\times10^{-5}$ for $\phi_{D,\rm II}^+$, respectively.