About the Project
25 Zeta and Related FunctionsRelated Functions

§25.11 Hurwitz Zeta Function

Contents
  1. §25.11(i) Definition
  2. §25.11(ii) Graphics
  3. §25.11(iii) Representations by the Euler–Maclaurin Formula
  4. §25.11(iv) Series Representations
  5. §25.11(v) Special Values
  6. §25.11(vi) Derivatives
  7. §25.11(vii) Integral Representations
  8. §25.11(viii) Further Integral Representations
  9. §25.11(ix) Integrals
  10. §25.11(x) Further Series Representations
  11. §25.11(xi) Sums
  12. §25.11(xii) a-Asymptotic Behavior

§25.11(i) Definition

The function \zeta\left(s,a\right) was introduced in Hurwitz (1882) and defined by the series expansion

25.11.1 \zeta\left(s,a\right)=\sum_{n=0}^{\infty}\frac{1}{(n+a)^{s}},\Re s>1, a\neq 0,-1,-2,\dots.

\zeta\left(s,a\right) has a meromorphic continuation in the s-plane, its only singularity in \mathbb{C} being a simple pole at s=1 with residue 1. As a function of a, with s (\neq 1) fixed, \zeta\left(s,a\right) is analytic in the half-plane \Re a>0. The Riemann zeta function is a special case:

25.11.2 \zeta\left(s,1\right)=\zeta\left(s\right).

For most purposes it suffices to restrict 0<\Re a\leq 1 because of the following straightforward consequences of (25.11.1):

25.11.3 \zeta\left(s,a\right)=\zeta\left(s,a+1\right)+a^{-s},
25.11.4 \zeta\left(s,a\right)=\zeta\left(s,a+m\right)+\sum_{n=0}^{m-1}\frac{1}{(n+a)^{%
s}},m=1,2,3,\dots.

Most references treat real a with 0<a\leq 1.

§25.11(ii) Graphics

See accompanying text
Figure 25.11.1: Hurwitz zeta function \zeta\left(x,a\right), a = 0.3, 0.5, 0.8, 1, -20\leq x\leq 10. The curves are almost indistinguishable for -14<x<-1, approximately. Magnify 3D Help
See accompanying text
Figure 25.11.2: Hurwitz zeta function \zeta\left(x,a\right), -19.5\leq x\leq 10, 0.02\leq a\leq 1. Magnify 3D Help

§25.11(iii) Representations by the Euler–Maclaurin Formula

25.11.6 \zeta\left(s,a\right)=\frac{1}{a^{s}}\left(\frac{1}{2}+\frac{a}{s-1}\right)-%
\frac{s(s+1)}{2}\int_{0}^{\infty}\frac{\widetilde{B}_{2}\left(x\right)-B_{2}}{%
(x+a)^{s+2}}\,\mathrm{d}x,s\neq 1, \Re s>-1, a>0.

For \widetilde{B}_{n}\left(x\right) see §24.2(iii).

§25.11(iv) Series Representations

25.11.8 \zeta\left(s,\tfrac{1}{2}a\right)=\zeta\left(s,\tfrac{1}{2}a+\tfrac{1}{2}%
\right)+2^{s}\sum_{n=0}^{\infty}\frac{(-1)^{n}}{(n+a)^{s}},\Re s>0, s\neq 1, 0<a\leq 1.
25.11.9 \zeta\left(1-s,a\right)=\frac{2\Gamma\left(s\right)}{(2\pi)^{s}}\*\sum_{n=1}^{%
\infty}\frac{1}{n^{s}}\cos\left(\tfrac{1}{2}\pi s-2n\pi a\right),\Re s>0 if 0<a<1; \Re s>1 if a=1.
25.11.10 \zeta\left(s,a\right)=\sum_{n=0}^{\infty}\frac{{\left(s\right)_{n}}}{n!}\zeta%
\left(n+s\right)(1-a)^{n},s\neq 1, |a-1|<1.

When a=\frac{1}{2}, (25.11.10) reduces to (25.8.3); compare (25.11.11).

For other series expansions similar to (25.11.10) see Coffey (2008).

§25.11(v) Special Values

Throughout this subsection \Re a>0.

25.11.11 \zeta\left(s,\tfrac{1}{2}\right)=(2^{s}-1)\zeta\left(s\right),s\neq 1.
25.11.12 \zeta\left(n+1,a\right)=\frac{(-1)^{n+1}{\psi}^{(n)}\left(a\right)}{n!},n=1,2,3,\dots.
25.11.13 \zeta\left(0,a\right)=\tfrac{1}{2}-a.
25.11.14 \zeta\left(-n,a\right)=-\frac{B_{n+1}\left(a\right)}{n+1},n=0,1,2,\dots.
25.11.15 \zeta\left(s,ka\right)=k^{-s}\*\sum_{n=0}^{k-1}\zeta\left(s,a+\frac{n}{k}%
\right),s\neq 1, k=1,2,3,\dots.
25.11.16 \zeta\left(1-s,\frac{h}{k}\right)=\frac{2\Gamma\left(s\right)}{(2\pi k)^{s}}\*%
\sum_{r=1}^{k}\cos\left(\frac{\pi s}{2}-\frac{2\pi rh}{k}\right)\zeta\left(s,%
\frac{r}{k}\right),s\neq 0,1; h,k integers, 1\leq h\leq k.

§25.11(vi) Derivatives

a-Derivative

25.11.17 \frac{\partial}{\partial a}\zeta\left(s,a\right)=-s\zeta\left(s+1,a\right),s\neq 0,1; \Re a>0.

s-Derivatives

In (25.11.18)–(25.11.24) primes on \zeta denote derivatives with respect to s. Similarly in §§25.11(viii) and 25.11(xii).

25.11.19 \zeta'\left(s,a\right)=-\frac{\ln a}{a^{s}}\left(\frac{1}{2}+\frac{a}{s-1}%
\right)-\frac{a^{1-s}}{(s-1)^{2}}+\frac{s(s+1)}{2}\int_{0}^{\infty}\frac{(%
\widetilde{B}_{2}\left(x\right)-B_{2})\ln\left(x+a\right)}{(x+a)^{s+2}}\,%
\mathrm{d}x-\frac{(2s+1)}{2}\int_{0}^{\infty}\frac{\widetilde{B}_{2}\left(x%
\right)-B_{2}}{(x+a)^{s+2}}\,\mathrm{d}x,\Re s>-1, s\neq 1, a>0.
25.11.20 (-1)^{k}{\zeta}^{(k)}\left(s,a\right)=\frac{(\ln a)^{k}}{a^{s}}\left(\frac{1}{%
2}+\frac{a}{s-1}\right)+k!a^{1-s}\sum_{r=0}^{k-1}\frac{(\ln a)^{r}}{r!(s-1)^{k%
-r+1}}-\frac{s(s+1)}{2}\int_{0}^{\infty}\frac{(\widetilde{B}_{2}\left(x\right)%
-B_{2})(\ln\left(x+a\right))^{k}}{(x+a)^{s+2}}\,\mathrm{d}x+\frac{k(2s+1)}{2}%
\int_{0}^{\infty}\frac{(\widetilde{B}_{2}\left(x\right)-B_{2})(\ln\left(x+a%
\right))^{k-1}}{(x+a)^{s+2}}\,\mathrm{d}x-\frac{k(k-1)}{2}\int_{0}^{\infty}%
\frac{(\widetilde{B}_{2}\left(x\right)-B_{2})(\ln\left(x+a\right))^{k-2}}{(x+a%
)^{s+2}}\,\mathrm{d}x,\Re s>-1, s\neq 1, a>0.
25.11.21 \zeta'\left(1-2n,\frac{h}{k}\right)=\frac{(\psi\left(2n\right)-\ln\left(2\pi k%
\right))B_{2n}\left(h/k\right)}{2n}-\frac{(\psi\left(2n\right)-\ln\left(2\pi%
\right))B_{2n}}{2nk^{2n}}+\frac{(-1)^{n+1}\pi}{(2\pi k)^{2n}}\sum_{r=1}^{k-1}%
\sin\left(\frac{2\pi rh}{k}\right){\psi}^{(2n-1)}\left(\frac{r}{k}\right)+%
\frac{(-1)^{n+1}2\cdot(2n-1)!}{(2\pi k)^{2n}}\sum_{r=1}^{k-1}\cos\left(\frac{2%
\pi rh}{k}\right)\zeta'\left(2n,\frac{r}{k}\right)+\frac{\zeta'\left(1-2n%
\right)}{k^{2n}},

where h,k are integers with 1\leq h\leq k and n=1,2,3,\dots.

25.11.22 \zeta'\left(1-2n,\tfrac{1}{2}\right)=-\frac{B_{2n}\ln 2}{n\cdot 4^{n}}-\frac{(%
2^{2n-1}-1)\zeta'\left(1-2n\right)}{2^{2n-1}},n=1,2,3,\dots.
25.11.24 \sum_{r=1}^{k-1}\zeta'\left(s,\frac{r}{k}\right)=(k^{s}-1)\zeta'\left(s\right)%
+k^{s}\zeta\left(s\right)\ln k,s\neq 1, k=1,2,3,\dots.

§25.11(vii) Integral Representations

25.11.27 \zeta\left(s,a\right)=\frac{1}{2}a^{-s}+\frac{a^{1-s}}{s-1}+\frac{1}{\Gamma%
\left(s\right)}\int_{0}^{\infty}\left(\frac{1}{e^{x}-1}-\frac{1}{x}+\frac{1}{2%
}\right)x^{s-1}e^{-ax}\,\mathrm{d}x,\Re s>-1, s\neq 1, \Re a>0.
25.11.28 \zeta\left(s,a\right)=\frac{1}{2}a^{-s}+\frac{a^{1-s}}{s-1}+\sum_{k=1}^{n}%
\frac{B_{2k}}{(2k)!}{\left(s\right)_{2k-1}}a^{1-s-2k}+\frac{1}{\Gamma\left(s%
\right)}\int_{0}^{\infty}\left(\frac{1}{e^{x}-1}-\frac{1}{x}+\frac{1}{2}-\sum_%
{k=1}^{n}\frac{B_{2k}}{(2k)!}x^{2k-1}\right)x^{s-1}e^{-ax}\,\mathrm{d}x,\Re s>-(2n+1), s\neq 1, \Re a>0.
25.11.30 \zeta\left(s,a\right)=\frac{\Gamma\left(1-s\right)}{2\pi i}\int_{-\infty}^{(0+%
)}\frac{e^{az}z^{s-1}}{1-e^{z}}\,\mathrm{d}z,s\neq 1, \Re a>0,

where the integration contour (see Figure 5.9.1) is a loop around the negative real axis as described for (25.5.20).

§25.11(viii) Further Integral Representations

25.11.31 \frac{1}{\Gamma\left(s\right)}\int_{0}^{\infty}\frac{x^{s-1}e^{-ax}}{2\cosh x}%
\,\mathrm{d}x=4^{-s}\left(\zeta\left(s,\tfrac{1}{4}+\tfrac{1}{4}a\right)-\zeta%
\left(s,\tfrac{3}{4}+\tfrac{1}{4}a\right)\right),\Re s>0, \Re a>-1.
25.11.32 \int_{0}^{a}x^{n}\psi\left(x\right)\,\mathrm{d}x=(-1)^{n-1}\zeta'\left(-n%
\right)+(-1)^{n}H_{n}\frac{B_{n+1}}{n+1}-\sum_{k=0}^{n}(-1)^{k}\genfrac{(}{)}{%
0.0pt}{}{n}{k}H_{k}\frac{B_{k+1}(a)}{k+1}a^{n-k}+\sum_{k=0}^{n}(-1)^{k}%
\genfrac{(}{)}{0.0pt}{}{n}{k}\zeta'\left(-k,a\right)a^{n-k},n=1,2,\dots, \Re a>0,

where H_{n} are the harmonic numbers:

25.11.33 H_{n}=\sum_{k=1}^{n}k^{-1}.

§25.11(ix) Integrals

See Prudnikov et al. (1990, §2.3), Prudnikov et al. (1992a, §3.2), and Prudnikov et al. (1992b, §3.2).

§25.11(x) Further Series Representations

25.11.35 \sum_{n=0}^{\infty}\frac{(-1)^{n}}{(n+a)^{s}}=\frac{1}{\Gamma\left(s\right)}%
\int_{0}^{\infty}\frac{x^{s-1}e^{-ax}}{1+e^{-x}}\,\mathrm{d}x=2^{-s}\left(%
\zeta\left(s,\tfrac{1}{2}a\right)-\zeta\left(s,\tfrac{1}{2}(1+a)\right)\right),\Re a>0, \Re s>0; or \Re a=0, \Im a\neq 0, 0<\Re s<1.

When a=1, (25.11.35) reduces to (25.2.3).

25.11.36 Removed because it is just (25.15.1) combined with (25.15.3).

See also (8.15.2) and Srivastava and Choi (2001).

§25.11(xi) Sums

25.11.37 \sum_{k=1}^{\infty}\frac{(-1)^{k}}{k}\zeta\left(nk,a\right)=-n\ln\Gamma\left(a%
\right)+\ln\left(\prod_{j=0}^{n-1}\Gamma\left(a-e^{(2j+1)\pi i/n}\right)\right),n=2,3,4,\dots, \Re a\geq 1.
25.11.39 \sum_{k=2}^{\infty}\frac{k}{2^{k}}\zeta\left(k+1,\tfrac{3}{4}\right)=8G,

where G is Catalan’s constant:

25.11.40 G\equiv\sum_{n=0}^{\infty}\frac{(-1)^{n}}{(2n+1)^{2}}=0.91596\;55941\;772\dots.

For further sums see Prudnikov et al. (1990, pp. 396–397) and Hansen (1975, pp. 358–360).

§25.11(xii) a-Asymptotic Behavior

As a\to 0 with s(\neq 1) fixed,

25.11.41 \zeta\left(s,a+1\right)=\zeta\left(s\right)-s\zeta\left(s+1\right)a+O\left(a^{%
2}\right).

As \beta\to\pm\infty with s fixed, \Re s>1,

25.11.42 \zeta\left(s,\alpha+i\beta\right)\to 0,

uniformly with respect to bounded nonnegative values of \alpha.

As a\to\infty in the sector |\operatorname{ph}a|\leq\pi-\delta(<\pi), with s(\neq 1) and \delta fixed, we have the asymptotic expansion

25.11.43 \zeta\left(s,a\right)-\frac{a^{1-s}}{s-1}-\frac{1}{2}a^{-s}\sim\sum_{k=1}^{%
\infty}\frac{B_{2k}}{(2k)!}{\left(s\right)_{2k-1}}a^{1-s-2k}.

Similarly, as a\to\infty in the sector |\operatorname{ph}a|\leq\pi-\delta(<\pi).

and

For the more general case \zeta'\left(-m,a\right), m=1,2,\dots, see Elizalde (1986). For error bounds for (25.11.43), (25.11.44) and (25.11.45), see Nemes (2017a).

For an exponentially-improved form of (25.11.43) see Paris (2005b).