Hankel Representation of Riemann Zeta Function

Theorem
Let $C$ be the Hankel contour.

Then for $s \in \C \setminus \Z_{>0}$:


 * $\displaystyle \zeta\left({s}\right) = \frac {i \Gamma \left({1 - s}\right)} {2 \pi} \oint_C \frac {\left({-z}\right)^{s - 1} } {e^z - 1} \, \mathrm d z$

where:
 * $\zeta$ is the Riemann Zeta function
 * $\Gamma$ is the Gamma function.