First make the substitution $z= e^{2u}$ to cast the integrand into the form $\frac{ e^{\beta u} \ du}{ \cosh^3 u}$ where $\beta$ is real.
Then note that in terms of the complex variable $w=u+iv$
$\cosh w = \cos (iw)$ is periodic with period $2\pi$ in $v$. This allows you to create a closed loop contour in the $w$ plane comprising two parallel horizontal lines. The loop encloses one singularity at $w= i\pi/2$. Thus you are reduced to computing a single residue, at that triple pole.
To find the residue at the triple pole you need to find a Laurent expansion. You can exploit the trig identity $\cos (\pi/2+ \zeta)= -\sin \zeta =- \zeta+ \ldots$ and cube this to determine the Laurent expansion of the integrand there.
Note that the two vertical segments in your contour are harmless if the denominator grows much faster than the numerator. This will be true for a restricted range of $\beta $ values.