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§25.14 Lerch’s Transcendent

Contents
  1. §25.14(i) Definition
  2. §25.14(ii) Properties

§25.14(i) Definition

25.14.1 {\Phi\left(z,s,a\right)\equiv\sum_{n=0}^{\infty}\frac{z^{n}}{(a+n)^{s}}},|z|<1; \Re s>1,|z|=1.

If s is not an integer then \left|\operatorname{ph}a\right|<\pi; if s is a positive integer then a\neq 0,-1,-2,\dots; if s is a non-positive integer then a can be any complex number. For other values of z, \Phi\left(z,s,a\right) is defined by analytic continuation. This is the notation used in Erdélyi et al. (1953a, p. 27). Lerch (1887) used \mathfrak{K}(a,x,s)=\Phi\left(e^{2\pi ix},s,a\right).

The Hurwitz zeta function \zeta\left(s,a\right)25.11) and the polylogarithm \operatorname{Li}_{s}\left(z\right)25.12(ii)) are special cases:

25.14.2 \zeta\left(s,a\right)=\Phi\left(1,s,a\right),\Re s>1, a\neq 0,-1,-2,\dots,
25.14.3 \operatorname{Li}_{s}\left(z\right)=z\Phi\left(z,s,1\right),\Re s>1, |z|\leq 1.

If s=m a positive integer then

Here the prime signifies that the term for n=m-1 is to be omitted. In the case s=1 we have

25.14.3_3 {a\Phi\left(z,1,a\right)=F\left(a,1;a+1;z\right)},\left|z\right|<1.

For hypergeometric function F see 15.2(i).

§25.14(ii) Properties

With the conditions of (25.14.1) and m=1,2,3,\dots,

25.14.4 \Phi\left(z,s,a\right)=z^{m}\Phi\left(z,s,a+m\right)+\sum_{n=0}^{m-1}\frac{z^{%
n}}{(a+n)^{s}}.
25.14.6 \Phi\left(z,s,a\right)=\frac{1}{2}a^{-s}+\int_{0}^{\infty}\frac{z^{x}}{(a+x)^{%
s}}\,\mathrm{d}x-2\int_{0}^{\infty}\frac{\sin\left(x\ln z-s\operatorname{%
arctan}\left(x/a\right)\right)}{(a^{2}+x^{2})^{s/2}(e^{2\pi x}-1)}\,\mathrm{d}x,\Re a>0 if \left|z\right|<1; \Re s>1, \Re a>0 if \left|z\right|=1.

Lerch’s transformation formula

For these and further properties see Erdélyi et al. (1953a, pp. 27–31).

25.14.8 \Phi\left(-z,s,a\right)=\frac{1}{2\pi\mathrm{i}}\int_{\sigma-\mathrm{i}\infty}%
^{\sigma+\mathrm{i}\infty}\frac{\Gamma\left(1+t\right)\Gamma\left(-t\right)z^{%
t}}{\left(a+t\right)^{s}}\,\mathrm{d}t,\left|\arg z\right|<\pi, \Re{a}>0,

with \max(-\Re{a},-1)<\sigma<0. This Mellin–Barnes integral representation is used in Olde Daalhuis (2024) to obtain large \left|z\right| asymptotic approximations for \Phi\left(-z,s,a\right). In the special case s=m an integer these asymptotic approximations simplify

The first sum is zero in the case that m is a non-positive integer. In the case that m is a positive integer we have the additional constraint a\not=1,2,3,\ldots. The coefficients b_{n} are the Taylor coefficients of \csc\left(\pi(t-a)\right) about t=0.

The small and large a asymptotics is discussed in Cai and López (2019), Ferreira and López (2004), Paris (2016), and the asymptotics as \Re{s}\to-\infty is discussed in Navas et al. (2013).