The Productions and Strong Decays of $D_q(2S)$ and $B_q(2S)$

Abstract

We study the productions of first radial excited states $D_q(2S)$ ($q=u,d,s$) and $B_q(2S)$ in exclusive semi-leptonic $B_{q^{\prime }}$ ($q^{\prime }=u,ds,c$) decays by the improved Bethe-Salpeter method. These 2S states can be detected through their strong decays to ground mesons, where the strong decays are calculated by the low energy approximation as well as the impulse approximation. Some channels have ratios of order $10^{-4}$: $Br(B^{+}\to {\bar{D}}^0(2S){\ell }^{+}{\nu }_{\ell })\times Br({\bar{D}}^0(2S)\to {\bar{D}}^{\ast }\pi )\approx (4.9\pm 4.0)\times 10^{-4}$, $Br(B^0\to D^{-}(2S){\ell }^{+}{\nu }_{\ell })\times Br(D^{-}(2S)\to {\bar{D}}^{\ast }\pi )\approx (4.4\pm 3.4)\times 10^{-4}$. These channels could be measured by the current B-factories. For $D_s(2S)$, we also obtain a relative large ratio: $Br(B_s^0\to D_s^{-}(2S){\ell }^{+}{\nu }_{\ell })\times Br(D_s^{-}(2S)\to {\bar{D}}^{\ast }\bar{K})\approx (9.9\pm 14.9)\times 10^{-4}$. Although there are discrepancies of the full decay width between the theoretical predictions of $D^0(2S)$ and experimental results of $D(2550{)}^0$, the new detected state $D(2550{)}^0$ is very likely the $D^0(2S)$ state.

Comments: 22 pages, 5 figures, 5 tables