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Related papers: Fuchs versus Painlev\'e

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We present two examples of reductions from the evolution equations describing discrete Schlesinger transformations of Fuchsian systems to difference Painlev\'e equations: difference Painlev\'e equation d-$P\left({A}_{2}^{(1)*}\right)$ with…

Mathematical Physics · Physics 2014-08-19 Anton Dzhamay , Tomoyuki Takenawa

We show how the unformizable representation for Abelian integrals of nontrivial genera arise. The technique makes use of the famous Chudnovsky's Fuchsian linear differential equations and their relation to the sixth Painleve transcendent.

Classical Analysis and ODEs · Mathematics 2012-10-16 Yu. V. Brezhnev

In this paper, we take ODE reductions of the general nonlinear Schr\"odinger equation (NLS) AKNS system, and reduce them to Painlev\'e type equations. Specifically, the stationary solution is solved in terms of elliptic functions, and the…

Exactly Solvable and Integrable Systems · Physics 2021-04-22 Jonathon Liu

In the enduring, fruitful research on spectral differential equations with polynomial eigenfunctions, Koornwinder's generalized Laguerre polynomials are playing a prominent role. Being orthogonal on the positive half-line with respect to…

Classical Analysis and ODEs · Mathematics 2017-08-02 Clemens Markett

We consider a 3-dimensional Pfaffian system, whose z-component is a differential system with irregular singularity at infinity and Fuchsian at zero. In the first part of the paper, we prove that its Frobenius integrability is equivalent to…

Classical Analysis and ODEs · Mathematics 2021-11-04 Gabriele Degano , Davide Guzzetti

We derive Fredholm determinant representation for isomonodromic tau functions of Fuchsian systems with $n$ regular singular points on the Riemann sphere and generic monodromy in $\mathrm{GL}(N,\mathbb C)$. The corresponding operator acts in…

Mathematical Physics · Physics 2018-10-30 P. Gavrylenko , O. Lisovyy

We consider a non-uniformly elliptic second-order differential operator with periodic coefficients that models composite media consisting of highly anisotropic cylindrical fibres periodically distributed in an isotropic background. The…

Analysis of PDEs · Mathematics 2025-08-01 Shane Cooper , Ilia Kamotski

The diagonal spin-spin correlations of the square lattice Ising model, originally expressed as Toeplitz determinants, are given by two distinct Fredholm determinants - one with an integral operator having an Appell function kernel and…

Classical Analysis and ODEs · Mathematics 2011-05-24 N. S. Witte , P. J. Forrester

It is shown that a generalization of the Painlev\'e-II equation (P-II) to a system of coupled equations with symmetry breaking terms is integrable. A Lax pair for this system is used to relate the asymptotic behavior of the solutions at…

Mathematical Physics · Physics 2026-03-30 N. A. Sinitsyn

We study underdetermined-elliptic linear partial differential operators $P$ on asymptotically Euclidean manifolds, such as the divergence operator on 1-forms or symmetric 2-tensors. Suitably interpreted, these are instances of (weighted)…

Analysis of PDEs · Mathematics 2025-08-18 Peter Hintz

We consider the Hankel determinant generated by the Gaussian weight with two jump discontinuities. Utilizing the results of [C. Min and Y. Chen, Math. Meth. Appl. Sci. {\bf 42} (2019), 301--321] where a second order PDE was deduced for the…

Mathematical Physics · Physics 2020-06-16 Shulin Lyu , Yang Chen

A two-parameter generalization of the complete elliptic integral of second kind is expressed in terms of the Appell function $F_{4}$. This function is further reduced to a quite simple bilinear form in the complete elliptic integrals $K$…

Mathematical Physics · Physics 2007-08-20 Victor Barsan

This paper is about elliptic and parabolic partial differential operators with discontinuities in the gradient which are compatible with a Finsler norm in a sense to be made precise. Examples of this type of problems arise in a number of…

Analysis of PDEs · Mathematics 2021-10-19 Peter S. Morfe , Panagiotis E. Souganidis

In our previous work, a unified description as polynomial Hamiltonian systems was established for a broad class of the Schlesinger systems including the sixth Painleve equation and Garnier systems. The main purpose of this paper is to…

Classical Analysis and ODEs · Mathematics 2010-09-15 Teruhisa Tsuda

This paper proves comparison principles for elliptic PDE involving the Finsler infinity Laplacian, a second-order differential operator with discontinuities in the gradient variable arising in $L^{\infty}$-variational problems and…

Analysis of PDEs · Mathematics 2024-05-10 Peter S. Morfe

Considering a certain interpolation problem, we derive a series of elliptic difference isomonodromic systems together with their Lax forms. These systems give a multivariate extension of the elliptic Painlev\'e equation.

Mathematical Physics · Physics 2017-09-05 Yasuhiko Yamada

We represent and analyze the general solution of the sixth Painleve transcendent in the Picard-Hitchin-Okamoto class in the Painleve form as the logarithmic derivative of the ratio of certain $\tau$-functions. These functions are…

Classical Analysis and ODEs · Mathematics 2010-11-18 Yurii V. Brezhnev

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

All Painlev\'e equations can be written as a time-dependent Hamiltonian system, and as such they admit a natural generalization to the case of several particles with an interaction of Calogero type (rational, trigonometric or elliptic).…

Mathematical Physics · Physics 2019-02-20 Marco Bertola , Mattia Cafasso , Vladimir Roubtsov

We consider systems of ordinary differential equations (ODEs) of the form ${\cal B}{\mathbf K}=0$, where $\cal B$ is a Hamiltonian operator of a completely integrable partial differential equation (PDE) hierarchy, and ${\mathbf K}=(K,L)^T$.…

Exactly Solvable and Integrable Systems · Physics 2014-05-13 P R Gordoa , A Pickering , M Senthilvelan