Suppose $f(n)$ is a periodic function with period $q$. Now from this paper we get that if $\displaystyle\sum_{n=1}^{q}f(n)=0$ then $\displaystyle\sum_{n=1}^{\infty}\frac{f(n)}{n}=-\frac{1}{q}\displaystyle\sum_{a=1}^{q}f(a)\psi(\frac{a}{q})$, where $\psi$ is digamma function.
My question is whether we can find a generalization of this or not? I mean:
$f(n)$ is a periodic function with period $q$, but $\displaystyle\sum_{n=1}^{q}f(n)$ may not be zero. In that case for $\Re(s)>1$ define $F(s)=\displaystyle\sum_{n=1}^{\infty}\frac{f(n)}{n^s}$. Of course we can write $F(s)$ as finite linear combination of special values of Hurwitz Zeta function. Apart from that, is there any way to write $F(s)$ as a finite sum (e.g. finite linear combination of special values of digamma function like previous case)?
Any suggestion or reference will be appreciated.