English

Painleve versus Fuchs

Mathematical Physics 2011-07-19 v3 Statistical Mechanics High Energy Physics - Theory math.MP Exactly Solvable and Integrable Systems

Abstract

The sigma form of the Painlev{\'e} VI equation contains four arbitrary parameters and generically the solutions can be said to be genuinely ``nonlinear'' because they do not satisfy linear differential equations of finite order. However, when there are certain restrictions on the four parameters there exist one parameter families of solutions which do satisfy (Fuchsian) differential equations of finite order. We here study this phenomena of Fuchsian solutions to the Painlev{\'e} equation with a focus on the particular PVI equation which is satisfied by the diagonal correlation function C(N,N) of the Ising model. We obtain Fuchsian equations of order N+1N+1 for C(N,N) and show that the equation for C(N,N) is equivalent to the NthN^{th} symmetric power of the equation for the elliptic integral EE. We show that these Fuchsian equations correspond to rational algebraic curves with an additional Riccati structure and we show that the Malmquist Hamiltonian p,qp,q variables are rational functions in complete elliptic integrals. Fuchsian equations for off diagonal correlations C(N,M)C(N,M) are given which extend our considerations to discrete generalizations of Painlev{\'e}.

Cite

@article{arxiv.math-ph/0602010,
  title  = {Painleve versus Fuchs},
  author = {S. Boukraa and S. Hassani and J. -M. Maillard and B. M. McCoy and J. -A. Weil and N. Zenine},
  journal= {arXiv preprint arXiv:math-ph/0602010},
  year   = {2011}
}

Comments

18 pages, Dedicated to the centenary of the publication of the Painleve VI equation in the Comptes Rendus de l'Academie des Sciences de Paris by Richard Fuchs in 1905