English

New exact solutions for the discrete fourth Painlev\'e equation

solv-int 2015-06-26 v1 Exactly Solvable and Integrable Systems

Abstract

In this paper we derive a number of exact solutions of the discrete equation xn+1xn1+xn(xn+1+xn1)=2znxn3+(η3δ2zn2)xn2+μ2(xn+zn+γ)(xn+znγ),\eqno(1)x_{n+1}x_{n-1}+x_n(x_{n+1}+x_{n-1})= {-2z_nx_n^3+(\eta-3\delta^{-2}-z_n^2)x_n^2+\mu^2\over (x_n+z_n+\gamma)(x_n+z_n-\gamma)},\eqno(1) where zn=nδz_n=n\delta and η\eta, δ\delta, μ\mu and γ\gamma are constants. In an appropriate limit (1) reduces to the fourth \p\ (PIV) equation \d2w\dz2=12w(\dw\dz)2+\tfr32w3+4zw2+2(z2α)w+βw,\eqno(2){\d^2w\over\d z^2} = {1\over2w}\left({\d w\over\d z}\right)^2+\tfr32w^3 + 4zw^2 + 2(z^2-\alpha)w +{\beta\over w},\eqno(2) where α\alpha and β\beta are constants and (1) is commonly referred to as the discretised fourth Painlev\'e equation. A suitable factorisation of (1) facilitates the identification of a number of solutions which take the form of ratios of two polynomials in the variable znz_n. Limits of these solutions yield rational solutions of PIV (2). It is also known that there exist exact solutions of PIV (2) that are expressible in terms of the complementary error function and in this article we show that a discrete analogue of this function can be obtained by analysis of (1).

Keywords

Cite

@article{arxiv.solv-int/9409002,
  title  = {New exact solutions for the discrete fourth Painlev\'e equation},
  author = {Andrew P. Bassom and Peter A. Clarkson},
  journal= {arXiv preprint arXiv:solv-int/9409002},
  year   = {2015}
}

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Tex file 14 pages

R2 v1 2026-07-22T20:07:50.502Z