English

Rational Solutions of the Painlev\'e-III Equation: Large Parameter Asymptotics

Classical Analysis and ODEs 2018-08-07 v1 Mathematical Physics Complex Variables math.MP Exactly Solvable and Integrable Systems

Abstract

The Painlev\'e-III equation with parameters Θ0=n+m\Theta_0=n+m and Θ=mn+1\Theta_\infty=m-n+1 has a unique rational solution u(x)=un(x;m)u(x)=u_n(x;m) with un(;m)=1u_n(\infty;m)=1 whenever nZn\in\mathbb{Z}. Using a Riemann-Hilbert representation proposed in \cite{BothnerMS18}, we study the asymptotic behavior of un(x;m)u_n(x;m) in the limit n+n\to+\infty with mCm\in\mathbb{C} held fixed. We isolate an eye-shaped domain EE in the y=n1xy=n^{-1}x plane that asymptotically confines the poles and zeros of un(x;m)u_n(x;m) for all values of the second parameter mm. We then show that unless mm is a half-integer, the interior of EE is filled with a locally uniform lattice of poles and zeros, and the density of the poles and zeros is small near the boundary of EE but blows up near the origin, which is the only fixed singularity of the Painlev\'e-III equation. In both the interior and exterior domains we provide accurate asymptotic formul\ae\ for un(x;m)u_n(x;m) that we compare with un(x;m)u_n(x;m) itself for finite values of nn to illustrate their accuracy. We also consider the exceptional cases where mm is a half-integer, showing that the poles and zeros of un(x;m)u_n(x;m) now accumulate along only one or the other of two "eyebrows", i.e., exterior boundary arcs of EE.

Keywords

Cite

@article{arxiv.1808.01421,
  title  = {Rational Solutions of the Painlev\'e-III Equation: Large Parameter Asymptotics},
  author = {Thomas Bothner and Peter D. Miller},
  journal= {arXiv preprint arXiv:1808.01421},
  year   = {2018}
}

Comments

70 pages, 36 figures

R2 v1 2026-06-23T03:24:20.338Z