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On the Solution of a Painlev\'e III Equation

solv-int 2007-05-23 v1 Functional Analysis Exactly Solvable and Integrable Systems

Abstract

In a 1977 paper of McCoy, Tracy and Wu there appeared for the first time the solution of a Painlev\'e equation in terms of Fredholm determinants of integral operators. This equation is ψ(t)+t1ψ(t)=(1/2)sinh2ψ+2αt1sinhψ\psi''(t)+t^{-1}\psi'(t)=(1/2) \sinh 2\psi+2\alpha t^{-1} \sinh\psi, a special case of the Painlev\'e III equation. The proof in the cited paper is complicated, and the purpose of this note is to give a more straightforward one. First we give an equivalent formulation of the solution in terms of the kernel et(x+x1)/2x+yx1x+12α{e^{-t (x+x^{-1})/2}\over x+y}\Big|{x-1\over x+1}\Big|^{2\alpha}. There are already in the literature relatively simple proofs of the fact that when α=0\alpha=0 Fredholm determinants of this kernel give solutions to the equation. We extend this result here to general α\alpha.

Cite

@article{arxiv.solv-int/9808015,
  title  = {On the Solution of a Painlev\'e III Equation},
  author = {Harold Widom},
  journal= {arXiv preprint arXiv:solv-int/9808015},
  year   = {2007}
}

Comments

LaTeX file. 9 pages

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