Dilogarithm

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Short description: Special case of the polylogarithm
The dilogarithm along the real axis

In mathematics, the dilogarithm (or Spence's function), denoted as Li2(z), is a particular case of the polylogarithm. Two related special functions are referred to as Spence's function, the dilogarithm itself:

Li2(z)=0zln(1u)uduz

and its reflection. For |z| < 1, an infinite series also applies (the integral definition constitutes its analytical extension to the complex plane):

Li2(z)=k=1zkk2.

Alternatively, the dilogarithm function is sometimes defined as

1vlnt1tdt=Li2(1v).

In hyperbolic geometry the dilogarithm can be used to compute the volume of an ideal simplex. Specifically, a simplex whose vertices have cross ratio z has hyperbolic volume

D(z)=ImLi2(z)+arg(1z)log|z|.

The function D(z) is sometimes called the Bloch-Wigner function.[1] Lobachevsky's function and Clausen's function are closely related functions.

William Spence, after whom the function was named by early writers in the field, was a Scottish mathematician working in the early nineteenth century.[2] He was at school with John Galt,[3] who later wrote a biographical essay on Spence.

Analytic structure

Using the former definition above, the dilogarithm function is analytic everywhere on the complex plane except at z=1, where it has a logarithmic branch point. The standard choice of branch cut is along the positive real axis (1,). However, the function is continuous at the branch point and takes on the value Li2(1)=π2/6.

Identities

Li2(z)+Li2(z)=12Li2(z2).[4]
Li2(1z)+Li2(11z)=(lnz)22.[5]
Li2(z)+Li2(1z)=π26lnzln(1z).[4]
Li2(z)Li2(1z)+12Li2(1z2)=π212lnzln(z+1).[5]
Li2(z)+Li2(1z)=π26(ln(z))22.[4]

Particular value identities

Li2(13)16Li2(19)=π218(ln3)26.[5]
Li2(13)13Li2(19)=π218+(ln3)26.[5]
Li2(12)+16Li2(19)=π218+ln2ln3(ln2)22(ln3)23.[5]
Li2(14)+13Li2(19)=π218+2ln2ln32(ln2)223(ln3)2. [5]
Li2(18)+Li2(19)=12(ln98)2.[5]
36Li2(12)36Li2(14)12Li2(18)+6Li2(164)=π2.

Special values

Li2(1)=π212.
Li2(0)=0.
Li2(12)=π212(ln2)22.
Li2(1)=ζ(2)=π26, where ζ(s) is the Riemann zeta function.
Li2(2)=π24iπln2.
Li2(512)=π215+12(ln5+12)2=π215+12arcsch22.
Li2(5+12)=π210ln25+12=π210arcsch22.
Li2(352)=π215ln25+12=π215arcsch22.
Li2(512)=π210ln25+12=π210arcsch22.

In particle physics

Spence's Function is commonly encountered in particle physics while calculating radiative corrections. In this context, the function is often defined with an absolute value inside the logarithm:

Φ(x)=0xln|1u|udu={Li2(x),x1;π2312(lnx)2Li2(1x),x>1.

See also

Notes

References

Further reading

  • Bloch, Spencer J. (2000). Higher regulators, algebraic K-theory, and zeta functions of elliptic curves. CRM Monograph Series. 11. Providence, RI: American Mathematical Society. ISBN 0-8218-2114-8.