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It is well known that the sixth Painlev\'e equation $\PVI$ admits a group of B\"acklund transformations which is isomorphic to the affine Weyl group of type $\mathrm{D}_4^{(1)}$. Although various aspects of this unexpectedly large symmetry…

Algebraic Geometry · Mathematics 2017-10-20 Michi-aki Inaba , Katsunori Iwasaki , Masa-Hiko Saito

We present a method of determining a Lax representation for similarity reductions of autonomous and non-autonomous partial difference equations. This method may be used to obtain Lax representations that are general enough to provide the…

Exactly Solvable and Integrable Systems · Physics 2013-08-22 C. M. Ormerod , Peter H. van der Kamp , G. R. W. Quispel

Symmetries and solutions of the Painleve IV equation are presented in an alternative framework which provides the bridge between the Hamiltonian formalism and the symmetric Painleve IV equation. This approach originates from a method…

Mathematical Physics · Physics 2009-09-22 H. Aratyn , J. F. Gomes , A. H. Zimerman

We present a geometric description, based on the affine Weyl group E_{6}^{(1)}, of two discrete analogues of the Painlev\'e VI equation, known as the asymmetric q-P_{V} and asymmetric d-P_{IV}. This approach allows us to describe in a…

Exactly Solvable and Integrable Systems · Physics 2015-06-26 B. Grammaticos , A. Ramani , Y. Ohta

We examine quantum extensions of the continuous Painlev\'e equations, expressed as systems of first-order differential equations for non-commuting objects. We focus on the Painlev\'e equations II, IV and V. From their auto-B\"acklund…

Quantum Algebra · Mathematics 2010-12-17 Hajime Nagoya , Basil Grammaticos , Alfred Ramani

It is known that discrete Painlev\'e equations have symmetries of the affine Weyl groups. In this paper we propose a new representation of discrete Painlev\'e equations in which the symmetries become clearly visible. We know how to obtain…

Exactly Solvable and Integrable Systems · Physics 2007-05-23 Mikio Murata

A discretization of Painlev\'e VI equation was obtained by Jimbo and Sakai in 1996. There are two ways to quantize it: 1) use the affine Weyl group symmetry (of $D_5^{(1)}$) (Hasegawa, 2011), 2) Lax formalism i.e. monodromy preserving point…

Quantum Algebra · Mathematics 2015-06-11 Koji Hasegawa

We consider solutions of a discrete Painlev\'e equation arising from a construction of quantum minimal surfaces by Arnlind, Hoppe and Kontsevich, and in earlier work of Cornalba and Taylor on static membranes. While the discrete equation…

Mathematical Physics · Physics 2025-10-28 Peter A. Clarkson , Anton Dzhamay , Andrew N. W. Hone , Ben Mitchell

We propose quantum Painlev\'e systems of type $A_l^{(1)}$. These systems, for $l=1$ and $l\ge 2$, should be regarded as quantizations of the second Painlev\'e equation and the differential systems with the affine Weyl group symmetries of…

Quantum Algebra · Mathematics 2007-05-23 Hajime Nagoya

An overview is given on recent developments in the affine Weyl group approach to Painlev\'e equations and discrete Painlev\'e equations, based on the joint work with Y. Yamada and K. Kajiwara.

Mathematical Physics · Physics 2007-05-23 Masatoshi Noumi

We show the relation of the non-stationary difference equation proposed by one of the authors and the quantized discrete Painlev\'e VI equation. The five-dimensional Seiberg-Witten curve associated with the difference equation has a…

Exactly Solvable and Integrable Systems · Physics 2023-11-10 Hidetoshi Awata , Koji Hasegawa , Hiroaki Kanno , Ryo Ohkawa , Shamil Shakirov , Jun'ichi Shiraishi , Yasuhiko Yamada

We shall construct the quantized q-analogues of the birational Weyl group actions arising from nilpotent Poisson algebras, which are conceptual generalizations, proposed by Noumi and Yamada, of the B\"acklund transformations for Painlev\'e…

Quantum Algebra · Mathematics 2011-12-06 Gen Kuroki

We derive the discrete Painlev\'e equations associated to the affine Weyl group E$_8^{(1)}$ that can be represented by an (in the QRT sense) "asymmetric" trihomographic system. The method used in this paper is based on singularity…

Mathematical Physics · Physics 2020-03-18 Basil Grammaticos , Alfred Ramani , Ralph Willox , Junkichi Satsuma

We find four kinds of six-parameter family of coupled Painlev\'e VI systems in dimension four with affine Weyl group symmetry of types $B_6^{(1)}$, $D_6^{(1)}$ and $D_7^{(2)}$. Each system is the first example which gave higher-order…

Algebraic Geometry · Mathematics 2009-12-21 Yusuke Sasano

The Painlev\'e equations can be written as Hamiltonian systems with affine Weyl group symmetries. A canonical quantization of the Painlev\'e equations preserving the affine Weyl group symmetries has been studied. While, the Painlev\'e…

Mathematical Physics · Physics 2013-02-06 Hajime Nagoya , Yasuhiko Yamada

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

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 present an new system of ordinary differential equations with affine Weyl group symmetry of type E_6^{(1)}. This system is expressed as a Hamiltonian system of sixth order with a coupled Painleve VI Hamiltonian.

Mathematical Physics · Physics 2007-05-23 Kenta Fuji , Takao Suzuki

We construct a general quantization procedure for square integrable functions on well-behaved connected exponential Lie groups. The Lie groups in question should admit at least one co-adjoint orbit of maximal possible dimension. The…

Functional Analysis · Mathematics 2025-02-26 Stine Marie Berge , Simon Halvdansson

In the current paper we study auto-B\"acklund transformations of the non-stationary second Painlev\'e hierarchy $\text{P}_\text{II}^{(n)}$ depending on $n$ parameters: a parameter $\alpha_n$ and times $t_1, \dots, t_{n-1}$. Using generators…

Exactly Solvable and Integrable Systems · Physics 2023-10-10 Irina Bobrova
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