Some identities with the Riemann zeta function Can someone either help derive or give a reference to the identities in Appendix B, page 27 of this, http://arxiv.org/pdf/1111.6290v2.pdf
Here is a reproduction of Appendix B from Klebanov, Pufu, Sachdev and Safdi's $2012$ preprint (v2) 'Renyi Entropies for Free Field Theories' (from the source at arxiv.org and hoping there is no problem citing it here...(RM)).

B Useful mathematical formulae
In this section we present some useful mathematical formulae.  We begin with zeta function identities.
For $0 < a \leq 1$ we have the identity
$$\tag{B.1}  \zeta(z, a) = \frac{2 \Gamma(1 - z)}{(2 \pi)^{1-z}} \left[\sin \frac{z \pi}{2} \sum_{n=1}^\infty \frac{\cos 2 \pi a n}{n^{1-z}}
   + \cos \frac{z \pi}{2} \sum_{n=1}^\infty \frac{\sin 2 \pi a n}{n^{1-z}} \right] \,$$
Taking derivatives at $z=0, -1, -2$ gives
\begin{align}
\zeta'(-2, a) &= - \frac{1}{4 \pi^2} \sum_{n=1}^\infty \frac{\cos 2 \pi a n}{n^3}
   - \frac{1}{4 \pi^3} \sum_{n=1}^\infty \frac{(2 \log (2 \pi n) + 2 \gamma - 3) \sin 2 \pi a n}{n^3} \,, \\
  \tag{B.2}\zeta'(-1, a) &= \frac{1}{4 \pi} \sum_{n=1}^\infty \frac{\sin 2 \pi q n}{n^2}
   - \frac{1}{2 \pi^2} \sum_{n=1}^\infty \frac{(\log (2 \pi n) + \gamma - 1) \cos 2 \pi a n}{n^2} \,, \\
  \zeta'(0, a) &= \frac{1}{2} \sum_{n=1}^\infty \frac{\cos 2 \pi a n}{n}
   + \frac{1}{\pi} \sum_{n=1}^\infty \frac{(\log (2 \pi n) + \gamma) \sin 2 \pi a n}{n} \,.
\end{align}
Two other useful identities are the regularized sums
\begin{align}
   \tag{B.3}\sum_{n \in \mathbb{Z}} \log \left( \frac{n^2}{q^2} + a^2 \right)
   &=  2 \log \left[2 \sinh (\pi q |a|) \right] \,, \\
   \sum_{n \in \mathbb{Z} + \frac 12} \log \left(\frac{n^2}{q^2} + a^2 \right)
   &=  2 \log \left[2 \cosh (\pi q |a|) \right] \,.
\end{align}
These sums follow from the more general formula
$$\tag{B.4}\sum_{n \in \mathbb{Z}} \log \left( \frac{(n + \alpha)^2}{q^2} + a^2 \right)
   =  \log \left[2 \cosh (2 \pi q |a|) - 2 \cos (2 \pi \alpha)  \right] \,.$$
This relation in turn follows from the Poisson summation formula
$$\tag{B.5} \frac{1}{ 2 \pi q} \sum_{n \in \mathbb{Z}} \hat f \left( \frac{n + \alpha}{q} \right) =\sum_{k \in \mathbb{Z}} e^{-i 2 \pi k \alpha} f(2 \pi q k)  \,$$
applied to
$$\tag{B.6}\hat f(\omega)  = \log \left( \omega^2 + a^2 \right) \,.$$
For $t \neq 0$ one can simply calculate the inverse Fourier transform of $\hat f$:
$$\tag{B.7}f(t) = \int_{-\infty}^\infty \frac{d\omega}{2 \pi} e^{-i \omega t} \log \left(\omega^2 +a^2 \right) = - \frac{e^{-|a|\;|t|}}{|t|}  \,.$$
The case $t=0$ requires special care because the expression for $f(0)$ is divergent and requires regularization:
$$\tag{B.8}f(0) = \int_{-\infty}^\infty \frac{d\omega}{2 \pi} \log \left(\omega^2 +a^2 \right)
   = -\frac{d}{ds} \int \frac{d\omega}{2 \pi} \frac{1}{\left(\omega^2 +a^2 \right)^s} \Biggr\rvert_{s=0}
    = |a| \,.$$
Using $(B.6)-(B.8)$ one can show that $(B.5)$ reduces to $(B.4)$.

The first identity is essentially the functional equation for the Hurwitz Zeta Function. You can find a proof and associated results here, where the identity appears on page 2 of the pdf (pg 1916) as equation (2) where the $F$ series is defined on the previous page.
