Abstract

We show that the integral J(t)=(1/π3)∫0π∫0π∫0πdxdydzlog⁡(t−cos⁡x−cos⁡y−cos⁡z+cos⁡xcos⁡ycos⁡z)J(t) = (1/π^3) \int_0^π\int_0^π\int_0^πdx dy dz \log(t - \cos{x} - \cos{y} - \cos{z} + \cos{x}\cos{y}\cos{z}), can be expressed in terms of 5F4{_5F_4} hypergeometric functions. The integral arises in the solution by Baxter and Bazhanov of the free-energy of the sl(n)sl(n) Potts model, which includes the term J(2)J(2). Our result immediately gives the logarithmic Mahler measure of the Laurent polynomial k−(x+1/x)−(y+1/y)−(z+1/z)+1/4(x+1/x)(y+1/y)(z+1/z)k - (x+1/x) - (y+1/y) - (z+1/z) + 1/4(x+1/x) (y+1/y) (z+1/z) in terms of the same hypergeometric functions.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.