Electromagnetic Annihilation Rates of chi_(c0) and chi_(c2) with Both Relativistic and QCD Radiative Corrections

We estimate the electromagnetic decay rates of $\chi_{c0}\rightarrow \gamma\gamma$ and $\chi_{c2}\rightarrow\gamma\gamma$ by taking into account both relativistic and QCD radiative corrections. The decay rates are derived in the Bethe-Salpeter formalism and the QCD radiative corrections are included in accordance with factorization assumption. Using a QCD-inspired interquark potential, we obtain relativistic BS wavefunctions of $\chi_{c0}$ and $\chi_{c2}$ by solving BS equations for the corresponding $^{2S+1}L_J$ states. Our numerical result for the ratio $R=\frac{\Gamma(\chi_{c0}\rightarrow\gamma\gamma)}{\Gamma(\chi_{c2} \rightarrow\gamma\gamma)}$ is about $11-13$ which agrees with the update E760 experimental data. Explicit calculations show that the relativistic corrections due to spin-dependent interquark forces induced by gluon exchange enhance the ratio $R$ substantially and its value is insensitive to the choice of parameters that characterize the interquark potential. Our expressions for the decay widths are identical with that obtained in the NRQCD theory to the next-to-leading order in $v^2$ and $\alpha_s$. Moreover, we have determined two new coefficents in the nonperturbative matrix elements for these decay widths.