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§25.12 Polylogarithms

Contents

§25.12(i) Dilogarithms

The notation \mathop{\mathrm{Li}_{2}\/}\nolimits\!\left(z\right) was introduced in Lewin (1981) for a function discussed in Euler (1768) and called the dilogarithm in Hill (1828):

25.12.1\mathop{\mathrm{Li}_{2}\/}\nolimits\!\left(z\right)=\sum_{{n=1}}^{\infty}\frac%
{z^{n}}{n^{2}},|z|\leq 1.

Other notations and names for \mathop{\mathrm{Li}_{2}\/}\nolimits\!\left(z\right) include S_{2}(z) (Kölbig et al. (1970)), Spence function \mathrm{Sp}(z) (’t Hooft and Veltman (1979)), and \mathrm{L}_{2}(z) (Maximon (2003)).

In the complex plane \mathop{\mathrm{Li}_{2}\/}\nolimits\!\left(z\right) has a branch point at z=1. The principal branch has a cut along the interval [1,\infty) and agrees with (25.12.1) when |z|\leq 1; see also §4.2(i). The remainder of the equations in this subsection apply to principal branches.

When z=e^{{i\theta}}, 0\leq\theta\leq 2\pi, (25.12.1) becomes

The cosine series in (25.12.7) has the elementary sum

25.12.8\sum_{{n=1}}^{\infty}\frac{\mathop{\cos\/}\nolimits\!\left(n\theta\right)}{n^{%
2}}=\frac{\pi^{2}}{6}-\frac{\pi\theta}{2}+\frac{\theta^{2}}{4}.

By (25.12.2)

25.12.9\sum_{{n=1}}^{\infty}\frac{\mathop{\sin\/}\nolimits\!\left(n\theta\right)}{n^{%
2}}=-\int_{0}^{\theta}\mathop{\ln\/}\nolimits\!\left(2\mathop{\sin\/}\nolimits%
\!\left(\tfrac{1}{2}x\right)\right)dx.

The right-hand side is called Clausen’s integral.

For graphics see Figures 25.12.1 and 25.12.2, and for further properties see Maximon (2003), Kirillov (1995), Lewin (1981), Nielsen (1909), and Zagier (1989).

See accompanying text
Figure 25.12.1: Dilogarithm function \mathop{\mathrm{Li}_{2}\/}\nolimits\!\left(x\right), -20\leq x<1. Magnify
Figure 25.12.2: Absolute value of the dilogarithm function \left|\mathop{\mathrm{Li}_{2}\/}\nolimits\!\left(x+iy\right)\right|, -20\leq x\leq 20, -20\leq y\leq 20. Principal value. There is a cut along the real axis from 1 to \infty. Magnify

§25.12(ii) Polylogarithms

For real or complex s and z the polylogarithm \mathop{\mathrm{Li}_{{s}}\/}\nolimits\!\left(z\right) is defined by

25.12.10\mathop{\mathrm{Li}_{{s}}\/}\nolimits\!\left(z\right)=\sum_{{n=1}}^{\infty}%
\frac{z^{n}}{n^{s}}.

For each fixed complex s the series defines an analytic function of z for |z|<1. The series also converges when |z|=1, provided that \realpart{s}>1. For other values of z, \mathop{\mathrm{Li}_{{s}}\/}\nolimits\!\left(z\right) is defined by analytic continuation.

The notation \mathop{\phi\/}\nolimits\!\left(z,s\right) was used for \mathop{\mathrm{Li}_{{s}}\/}\nolimits\!\left(z\right) in Truesdell (1945) for a series treated in Jonquière (1889), hence the alternative name Jonquière’s function. The special case z=1 is the Riemann zeta function: \mathop{\zeta\/}\nolimits\!\left(s\right)=\mathop{\mathrm{Li}_{{s}}\/}%
\nolimits\!\left(1\right).

Integral Representation

valid when \realpart{s}>0 and \left|\mathop{\mathrm{ph}\/}\nolimits\!\left(1-z\right)\right|<\pi, or \realpart{s}>1 and z=1. (In the latter case (25.12.11) becomes (25.5.1)).

See also Lewin (1981), Kölbig (1986), Maximon (2003), Prudnikov et al. (1990, §§1.2 and 2.5), Prudnikov et al. (1992a, §3.3), and Prudnikov et al. (1992b, §3.3).

§25.12(iii) Fermi–Dirac and Bose–Einstein Integrals

The Fermi–Dirac and Bose–Einstein integrals are defined by

25.12.14F_{s}(x)=\frac{1}{\mathop{\Gamma\/}\nolimits\!\left(s+1\right)}\int_{0}^{%
\infty}\frac{t^{s}}{e^{{t-x}}+1}dt,s>-1,
25.12.15G_{s}(x)=\frac{1}{\mathop{\Gamma\/}\nolimits\!\left(s+1\right)}\int_{0}^{%
\infty}\frac{t^{s}}{e^{{t-x}}-1}dt,s>-1, x<0; or s>0, x\leq 0,

respectively. Sometimes the factor 1/\mathop{\Gamma\/}\nolimits\!\left(s+1\right) is omitted. See Cloutman (1989) and Gautschi (1993).

For a uniform asymptotic approximation for F_{s}(x) see Temme and Olde Daalhuis (1990).

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