Riemann zeta expansion about a=1

The Riemann zeta function is defined by the Dirichlet series

(1)   \begin{equation*}\zeta(s)=\sum_{n=1}^{\infty}\frac{1}{n^s}\end{equation*}


as a sum of reciprocal natural numbers raised to power s, which is absolutely convergent for \Re(s)>1and defined for a complex variable s=\sigma+it. Moreover, the \zeta extends meromorphically to \mathbb{C} having a simple pole at s=1 with residue 1, and there are many representations of \zeta valid in different domains and many in all \mathbb{C}\slash 1. The Laurent expansion about the pole is a common example

(2)   \begin{equation*}\zeta(s)=\frac{1}{s-1}+\sum_{n=0}^{\infty}\gamma_n\frac{(-1)^n(s-1)^n}{n!}\end{equation*}


of such a global representation, where its Stieltjes expansion coefficients are given by formula

(3)   \begin{equation*}\gamma_n=\lim_{k\to\infty}\Bigg{\sum_{m=1}^{k}\frac{\log^n(m)}{m}-\frac{\log^{n+1}(k)}{n+1}\Bigg}\end{equation*}


as k\to \infty, which is commonly written in the literature [3][3].