If the vertex factor for the decay of a vector boson $\mathrm{X}$ into two spin- $\frac{1}{2}$ fermions $\mathrm{f}_1$ and $\overline{\mathrm{f}}_2$ is
$$
-i g_X \gamma^\mu \frac{1}{2}\left(c_V-c_A \gamma^5\right),
$$
then show that
$$
\Gamma\left(X \rightarrow f_1 \hat{f}_2\right)=\frac{g_X^2}{48 \pi}\left(c_V^2+c_A^2\right) M_X,
$$
where $M_X$ is the mass of the boson and where we have neglected the masses of the fermions.