  The strong coupling constant is an important parameter which can help us to
understand the strong decay behaviors of baryons. In our previous work, we have
analyzed strong vertices $\Sigma_{c}^{*}ND$, $\Sigma_{b}^{*}NB$,
$\Sigma_{c}ND$, $\Sigma_{b}NB$ in QCD sum rules. Following these work, we
further analyze the strong vertices $\Sigma_{c}ND^{*}$ and $\Sigma_{b}NB^{*}$
using the three-point QCD sum rules under Dirac structures
$q\!\!\!/p\!\!\!/\gamma_{\alpha}$ and $q\!\!\!/p\!\!\!/p_{\alpha}$. In this
work, we first calculate strong form factors considering contributions of the
perturbative part and the condensate terms $\langle\overline{q}q\rangle$,
$\langle\frac{\alpha_{s}}{\pi}GG\rangle$ and $\langle\overline{q}g_{s}\sigma
Gq\rangle$. Then, these form factors are used to fit into analytical functions.
According to these functions, we finally determine the values of the strong
coupling constants for these two vertices $\Sigma_{c}ND^{*}$ and
$\Sigma_{b}NB^{*}$.
