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In this work we show that the $ N\times N $ Toeplitz determinants with the symbols $ z^{\mu}\exp(-{1/2}\sqrt{t}(z+1/z)) $ and $ (1+z)^{\mu}(1+1/z)^{\nu}\exp(tz) $ -- known $\tau$-functions for the \PIIIa and \PV systems -- are characterised…

Mathematical Physics · Physics 2007-05-23 P. J. Forrester , N. S. Witte

In this paper, we consider polynomials associated with faces and internal quadrilaterals of a cuboctahedron and classify them under the requirement that they are consistent. These polynomials give rise to a system of partial difference…

Exactly Solvable and Integrable Systems · Physics 2020-11-23 Nalini Joshi , Nobutaka Nakazono

This paper concerns the discrete version of the Painlev\'e identification problem, i.e., how to recognize a certain recurrence relation as a discrete Painlev\'e equation. Often some clues can be seen from the setting of the problem, e.g.,…

Exactly Solvable and Integrable Systems · Physics 2025-03-18 Xing Li , Anton Dzhamay , Galina Filipuk , Da-jun Zhang

We consider lattice equations on ${\mathds{Z}}^2$ which are autonomous, affine linear and possess the symmetries of the square. Some basic properties of equations of this type are derived, as well as a sufficient linearization condition and…

Exactly Solvable and Integrable Systems · Physics 2009-11-13 A. Tongas , D. Tsoubelis , P. Xenitidis

In this letter we establish a connection of Picard-type elliptic solutions of Painleve VI equation with the special solutions of the non-stationary Lame equation. The latter appeared in the study of the ground state properties of Baxter's…

High Energy Physics - Theory · Physics 2009-11-11 Vladimir V Bazhanov , Vladimir V Mangazeev

Two discretizations, linear and nonlinear, of basic notions of the complex analysis are considered. The underlying lattice is an arbitrary quasicrystallic rhombic tiling of a plane. The linear theory is based on the discrete Cauchy-Riemann…

Differential Geometry · Mathematics 2007-06-13 Alexander I. Bobenko , Christian Mercat , Yuri B. Suris

The G-function associated to the semi-simple Frobenius manifold C^n/W (where W is a Coxeter group or an extended affine Weyl group) is studied. The general form of the G function is given in terms of a logarithmic singularity over caustics…

Mathematical Physics · Physics 2020-12-15 I. A. B. Strachan

Over forty years ago, Paneitz, and independently Fradkin and Tseytlin, discovered a fourth-order conformally-invariant differential operator, intrinsically defined on a conformal manifold, mapping scalars to scalars. This operator is a…

Differential Geometry · Mathematics 2023-03-03 Samuel Blitz , A. Rod Gover , Andrew Waldron

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 new Lax pair for the sixth Painlev\'e equation $P_{VI}$ is constructed in the framework of the loop algebra $\mathfrak{so}(8)[z,z^{-1}]$. The whole affine Weyl group symmetry of $P_{VI}$ is interpreted as gauge transformations of the…

Mathematical Physics · Physics 2007-05-23 Masatoshi Noumi , Yasuhiko Yamada

We present a linear system of difference equations whose entries are expressed in terms of theta functions. This linear system is singular at $4m+12$ points for $m \geq 1$, which appear in pairs due to a symmetry condition. We parameterize…

Mathematical Physics · Physics 2017-09-13 Christopher M. Ormerod , Eric M. Rains

We study topological aspects of a compact lattice superconductor, and show that the characteristic energy splitting, $\Delta$, between almost degenerate ground states, is simply related to a novel order parameter $\tilde W$, which is…

Superconductivity · Physics 2007-05-23 Anders Vestergren , Jack Lidmar , T. H. Hansson

We analyze the Wigner function constructed on the basis of the discrete rotation and displacement operators labeled with elements of the underlying finite field. We separately discuss the case of odd and even characteristics and analyze the…

Quantum Physics · Physics 2007-05-23 A. B. Klimov , C. Munoz , J. L. Romero

We show that the Painlev{\'e} VI equation has an equivalent form of the non-autonomous Zhukovsky-Volterra gyrostat. This system is a generalization of the Euler top in $C^3$ and include the additional constant gyrostat momentum. The…

Quantum Algebra · Mathematics 2009-11-11 A. Levin , M. Olshanetsky , A. Zotov

The Wigner function provides a useful quasiprobability representation of quantum mechanics, with applications in various branches of physics. Many nice properties of the Wigner function are intimately connected with the high symmetry of the…

Quantum Physics · Physics 2016-02-03 Huangjun Zhu

In this paper, we study special solutions of five autonomous integrable partial difference equations (P$\Delta$Es). More precisely, we show that these P$\Delta$Es admit special solutions that are described by non-autonomous ordinary…

Exactly Solvable and Integrable Systems · Physics 2026-05-04 Nobutaka Nakazono

This paper explores the embedding of lattice structures $L \subseteq \mathbb{R}^n$ into smooth manifolds $M \subseteq \mathbb{R}^n$ through a rigorous mathematical framework. Building upon the foundational results established in "Embedding…

Analysis of PDEs · Mathematics 2025-12-02 Francesco D'Agostino

We study Brown's definition of the probabilistic zeta function of a finite lattice as a generalization of that of a finite group. We propose a natural alternative or extension that may be better suited for non-atomistic lattices. The…

Combinatorics · Mathematics 2024-10-03 Besfort Shala

Scaling symmetry of gl_n-type Drinfel'd-Sokolov hierarchy is investigated. Applying similarity reduction to the hierarchy, one can obtain the Schlesinger equation with (n+1) regular singularities. Especially in the case of n=3, the…

Exactly Solvable and Integrable Systems · Physics 2007-05-23 Saburo Kakei , Tetsuya Kikuchi

We propose a new representation of the fourth Painlev\'e equation in which the $A^{(1)}_2$-symmetries become clearly visible. By means of this representation, we clarify the internal relation between the fourth Painlev\'e equation and the…

q-alg · Mathematics 2008-02-03 Masatoshi Noumi , Yasuhiko Yamada