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We study the rational solutions of the discrete version of Painleve's fourth equation d-PIV. The solutions are generated by applying Schlesinger transformations on the seed solutions -2z and -1/z. After studying the structure of these…

solv-int · Physics 2008-02-03 Jarmo Hietarinta , Kenji Kajiwara

The third Painlev\'e equation in its generic form, often referred to as Painlev\'e-III($D_6$), is given by $$ \frac{{\rm d}^2u}{{\rm d}x^2} =\frac{1}{u}\left(\frac{{\rm d}u}{{\rm d}x}\right)^2-\frac{1}{x}\frac{{\rm d}u}{{\rm…

Classical Analysis and ODEs · Mathematics 2024-03-12 Ahmad Barhoumi , Oleg Lisovyy , Peter D. Miller , Andrei Prokhorov

It is well known that the Painlev\'e equations can formally degenerate to autonomous differential equations with elliptic function solutions in suitable scaling limits. A way to make this degeneration rigorous is to apply Deift-Zhou…

Mathematical Physics · Physics 2024-01-23 Robert J. Buckingham , Peter D. Miller

The Painlev\'e equations possess transcendental solutions $y(t)$ with special initial values that are symmetric under rotation or reflection in the complex $t$-plane. They correspond to monodromy problems that are explicitly solvable in…

Exactly Solvable and Integrable Systems · Physics 2023-04-26 Nalini Joshi , Pieter Roffelsen

We present the bilinear forms of the (continuous) Painlev\'e equations obtained from the continuous limit of the analogous expresssions for the discrete ones. The advantage of this method is that it leads to very symmetrical results. A new…

solv-int · Physics 2009-10-30 Y. Ohta , A. Ramani , B. Grammaticos , K. M. Tamizhmani

We show that the discrete Painlev\'e II equation with starting value $a_{-1}=-1$ has a unique solution for which $-1 < a_n < 1$ for every $n \geq 0$. This solution corresponds to the Verblunsky coefficients of a family of orthogonal…

Classical Analysis and ODEs · Mathematics 2024-01-17 Walter Van Assche

We present the discrete, q-, form of the Painlev\'e VI equation written as a three-point mapping and analyse the structure of its singularities. This discrete equation goes over to P_{VI} at the continuous limit and degenerates towards the…

solv-int · Physics 2007-05-23 B. Grammaticos , A. Ramani

We present particular solutions of the discrete Painlev\'e III (d-P$\rm_{III}$) equation of rational and special function (Bessel) type. These solutions allow us to establish a close parallel between this discrete equation and its…

solv-int · Physics 2009-10-22 B. Grammaticos , F. W. Nijhoff , V. Papageorgiou , A. Ramani

We consider orthogonal polynomials p_n with respect to an exponential weight function w(x) = exp(-P(x)). The related equations for the recurrence coefficients have been explored by many people, starting essentially with Laguerre [49], in…

Classical Analysis and ODEs · Mathematics 2016-09-06 Alphonse P. Magnus

Recurrence coefficients of semi-classical orthogonal polynomials (orthogonal polynomials related to a weight function $w$ such that $w'/w$ is a rational function) are shown to be solutions of non linear differential equations with respect…

Classical Analysis and ODEs · Mathematics 2016-09-06 Alphonse P. Magnus

This paper is an addendum to earlier papers \cite{R1,R2} in which it was shown that the unstable separatrix solutions for Painlev\'e I and II are determined by $PT$-symmetric Hamiltonians. In this paper unstable separatrix solutions of the…

Mathematical Physics · Physics 2021-08-05 Carl M. Bender , J. Komijani

Starting from the standard form of the five discrete Painlev\'e equations we show how one can obtain (through appropriate limits) a host of new equations which are also the discrete analogues of the continuous Painlev\'e equations. A…

solv-int · Physics 2015-06-26 A. Ramani , B. Grammaticos

By analogy to the continuous Painlev\'e II equation, we present particular solutions of the discrete Painlev\'e II (d-P$\rm_{II}$) equation. These solutions are of rational and special function (Airy) type. Our analysis is based on the…

solv-int · Physics 2009-10-28 J. Satsuma , K. Kajiwara , B. Grammaticos , J. Hietarinta , A. Ramani

We consider a class of particular solutions to the (2+1)-dimensional nonlinear partial differential equation (PDE) $u_t +\partial_{x_2}^n u_{x_1} - u_{x_1} u =0$ (here $n$ is any integer) reducing it to the ordinary differential equation…

Exactly Solvable and Integrable Systems · Physics 2015-06-15 A. I. Zenchuk

Hirota's discrete KdV equation is an integrable partial difference equation on $\mathbb{Z}^2$, which approaches the Korteweg-de Vries (KdV) equation in a continuum limit. In this paper, we show that its multiplicative-discrete versions have…

Exactly Solvable and Integrable Systems · Physics 2022-05-04 Nobutaka Nakazono

We obtain asymptotics of polynomials satisfying the orthogonality relations $$ \int_{\mathbb{R}} z^k P_n(z; t , N) \mathrm{e}^{-N \left(\frac{1}{4}z^4 + \frac{t}{2}z^2 \right)} \mathrm{d} z = 0 \quad \text{ for } \quad k = 0, 1, ..., n-1,…

Classical Analysis and ODEs · Mathematics 2024-06-25 Ahmad Barhoumi

The biharmonic supercritical equation $\Delta^2u=|u|^{p-1}u$, where $n>4$ and $p>(n+4)/(n-4)$, is studied in the whole space $\mathbb{R}^n$ as well as in a modified form with $\lambda(1+u)^p$ as right-hand-side with an additional eigenvalue…

Analysis of PDEs · Mathematics 2009-02-27 Alberto Ferrero , Hans-Christoph Grunau , Paschalis Karageorgis

The discrete Painlev\'e property is precisely defined, and basic discretization rules to preserve it are stated. The discrete Painlev\'e test is enriched with a new method which perturbs the continuum limit and generates infinitely many…

solv-int · Physics 2007-05-23 R. Conte , M. Musette

In this paper discrete equations are derived from B\"{a}cklund transformations of the fifth Painlev\'{e} equation, including a new discrete equation which has ternary symmetry. There are two classes of rational solutions of the fifth…

Exactly Solvable and Integrable Systems · Physics 2026-05-26 Peter A. Clarkson , Clare Dunning , Ben Mitchell

We use methods from dynamical systems to study the fourth Painleve equation PIV. Our starting point is the symmetric form of PIV, to which the Poincare compactification is applied. The motion on the sphere at infinity can be completely…

Exactly Solvable and Integrable Systems · Physics 2019-05-22 Jeremy Schiff , Michael Twiton
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