Semi-leptonic $B$ decays to tensor mesons

Abstract

Using the form factors of the transtions $B\to T$ with $T$ refering to a tensor meson, such as $a_2(1320), f_2(1270),K^*_2(1430), D_2^*(2460)$ and $D^*_{2s}(2573)$, within the covariant light-front quark model (CLFQM), we provide a detailed investigation of the corresponding semi-leptonic decays $B\to T\ell\nu_\ell$ with $\ell=e,\nu,\tau$. All the branching ratios of these decays are larger than $10^{-5}$, in which the maximum value can reach up to $10^{-3}$, indicating promising prospects for experimental observation. Furthermore, we also calculate the longitudinal polarization fractions $f_L$ and forward-backward asymmetries $A_{FB}$ for these considered decays. All the decays $B\to T \ell\nu_{\ell}$ are dominated by the longitudinal polarization, where the polarization fractions can reach up to $\sim70\%$ for the decays $B\to T \ell^{\prime}\nu_{\ell^\prime}$ with $\ell^\prime=e, \mu$, those of the decays $B\to T \tau\nu_{\tau}$ are a little smaller. The $A_{FB}$ values of the decays $B\to T \ell^{\prime}\nu_{\ell^\prime}$ and $B\to T \tau\nu_{\tau}$ have opposite signs.