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In this paper, we analyze the asymptotic behaviour of the poles of certain rational solutions of the fifth Painlev\'e equation. These solutions are constructed by relating the corresponding tau function to a Hankel determinant of a certain…

Exactly Solvable and Integrable Systems · Physics 2025-11-18 Malik Balogoun , Marco Bertola

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

We show that the Painleve equations P3-P5 can be derived (in a unified way) from a periodic sequence of Darboux transformations for a Schrodinger problem with quadratic eigenvalue dependency. The general problem naturally divides into three…

Exactly Solvable and Integrable Systems · Physics 2009-11-10 Ralph Willox , Jarmo Hietarinta

The problem of Painleve classification of ordinary differential equations lasting since the end of XIX century saw significant advances for the limited equation order, however not that much for the equations of higher orders. In this work…

Classical Analysis and ODEs · Mathematics 2014-10-13 Stanislav Sobolevsky

This article deals with the asymptotic behavior of fourth order differential equation where the coefficients are perturbations of linear constant coefficient equation. We introduce a change of variable and deduce that the new variable…

Classical Analysis and ODEs · Mathematics 2014-10-14 Anibal Coronel , Fernando Huancas , Manuel Pinto

We consider a $q$-Painlev\'e IV equation which is the $A_4^{(1)}$-surface type in the Sakai's classification. We find three distinct types of classical solutions with determinantal structures whose elements are basic hypergeometric…

Exactly Solvable and Integrable Systems · Physics 2014-08-25 Nobutaka Nakazono

For an arbitrary ordinary second order differential equation a test is constructed that checks if this equation is equivalent to Painleve I, II or Painleve III with three zero parameters equations under the substitutions of variables. If it…

Classical Analysis and ODEs · Mathematics 2009-09-11 V. V. Kartak

We classify rational solutions of a specific type of the set theoretical version of the pentagon equation. That is, we find all quadrirational maps $R:(x,y)\mapsto (u(x,y),v(x,y)),$ where $u, v$ are two rational functions on two arguments,…

Exactly Solvable and Integrable Systems · Physics 2024-09-27 Charalampos Evripidou , Pavlos Kassotakis , Anastasios Tongas

In this paper rational solutions of the fifth Painlev\'e equation are discussed. There are two classes of rational solutions of the fifth Painlev\'e equation, one expressed in terms of the generalised Laguerre polynomials, which are the…

Exactly Solvable and Integrable Systems · Physics 2024-01-15 Peter A. Clarkson , Clare Dunning

We provide a complete classification and an explicit representation of rational solutions to the fourth Painlev\'e equation PIV and its higher order generalizations known as the $A_{2n}$-Painlev\'e or Noumi-Yamada systems. The construction…

Mathematical Physics · Physics 2021-04-13 David Gómez-Ullate , Yves Grandati , Robert Milson

In this paper, we show that the B\"acklund transformations of Painlev\'e equations come from birational maps of rational surfaces constructed by Okamoto as the spaces of initial conditions. The simultaneous resolutions of rational double…

Algebraic Geometry · Mathematics 2017-10-20 Masa-Hiko Saito , Hiroshi Umemura

We present a general scheme to derive higher-order members of the Painleve VI (PVI) hierarchy of ODE's as well as their difference analogues. The derivation is based on a discrete structure that sits on the background of the PVI equation…

Exactly Solvable and Integrable Systems · Physics 2007-05-23 F. W. Nijhoff , A. J. Walker

A $\tau$ function formalism for Sakai's elliptic Painlev'e equation is presented. This establishes the equivalence between the two formulations by Sakai and by Ohta-Ramani-Grammaticos. We also give a simple geometric description of the…

Exactly Solvable and Integrable Systems · Physics 2007-05-23 Kenji Kajiwara , Masatoshi Noumi , Tetsu Masuda , Yasuhiro Ohta , Yasuhiko Yamada

A proposed solution to the Riemann Hypothesis

General Mathematics · Mathematics 2013-09-24 Gerasimos Pergaris

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

This paper gives parametric solutions to quartic equations of the type,(4-3-3),(4-4-4),(4-5-5) and (4-6-6), According to Lander, Parkin, and Selfridge (2) conjecture, there are non-trivial solutions of the quartic…

General Mathematics · Mathematics 2022-06-16 Seiji Tomita , Oliver Couto

The $2\times 2$ Schlesinger system for the case of four regular singularities is equivalent to the Painlev\'e VI equation. The Painlev\'e VI equation can in turn be rewritten in the symmetric form of Okamoto's equation; the dependent…

Exactly Solvable and Integrable Systems · Physics 2014-11-20 D. Korotkin , H. Samtleben

Among the reductions of the resonant three-wave interaction system to six-dimensional differential systems, one of them has been specifically mentioned as being linked to the generic sixth Painleve' equation P6. We derive this link…

Exactly Solvable and Integrable Systems · Physics 2014-06-26 Robert Conte , A. Michel Grundland , Micheline Musette

In this paper, we study Riccati solutions of Painlev\'e equations from a view point of geometry of Okamoto-Painlev\'e pairs $(S,Y)$. After establishing the correspondence between (rational) nodal curves on $S-Y$ and Riccati solutions, we…

Algebraic Geometry · Mathematics 2007-05-23 Masa-Hiko Saito , Hitomi Terajima

Painleve equations belong to the class y'' + a_1 {y'}^3 + 3 a_2 {y'}^2 + 3 a_3 y' + a_4 = 0, where a_i=a_i(x,y). This class of equations is invariant under the general point transformation x=Phi(X,Y), y=Psi(X,Y) and it is therefore very…

Exactly Solvable and Integrable Systems · Physics 2015-06-26 Jarmo Hietarinta , Valery Dryuma