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Recently, Feh\'er and Kluck discovered, at the level of classical mechanics, new compactified trigonometric Ruijsenaars-Schneider $n$-particle systems, with phase space symplectomorphic to the $(n-1)$-dimensional complex projective space.…

Mathematical Physics · Physics 2018-08-01 Tamás F. Görbe , Martin A. Hallnäs

For the Kirillov-Poisson structure on the vector space $\g^*$, where $\g$ is a finite-dimensional Lie algebra, it is known at least two canonical deformations quantization of this structure: they are the M. Kontsevich universal formula [K],…

Quantum Algebra · Mathematics 2007-05-23 Boris Shoikhet

We consider the problem of designing a variety of "system guided" basis sets for quantum mechanical anharmonic oscillators. Using ideas based on supersymmetric quantum mechanics, we design canonical transformations of the usual position and…

Quantum Physics · Physics 2017-01-12 Donald J. Kouri , Cameron L. Williams , Nikhil Pandyaq

In this paper we present canonical and canonoid transformations considered as global geometrical objects for Hamiltonian systems. Under the mathematical formalisms of symplectic, cosymplectic, contact and cocontact geometry, the canonoid…

Mathematical Physics · Physics 2023-03-15 R. Azuaje , A. M. Escobar-Ruiz

We consider an Ansatz for the study of the existence of formal integrals of motion for Kahan-Hirota-Kimura discretizations. In this context, we give a combinatorial proof of the formula of Celledoni-McLachlan-Owren-Quispel for an integral…

Exactly Solvable and Integrable Systems · Physics 2016-11-09 René Zander

Integrable Killing tensors are used to classify orthogonal coordinates in which the classical Hamilton-Jacobi equation can be solved by a separation of variables. We completely solve the Nijenhuis integrability conditions for Killing…

Differential Geometry · Mathematics 2014-07-30 Konrad Schöbel

In this paper, we apply the geometric Hamilton--Jacobi theory to obtain solutions of Hamiltonian systems in Classical Mechanics, that are either compatible with a cosymplectic or a contact structure. As it is well known, the first structure…

Mathematical Physics · Physics 2016-07-06 M. de León , C. Sardón

To any finite group G of automorphisms of a symplectic vector space V we associate a new multi-parameter deformation, H_k, of the smash product of G with the polynomial algebra on V. The algebra H_k, called a symplectic reflection algebra,…

Algebraic Geometry · Mathematics 2007-05-23 Pavel Etingof , Victor Ginzburg

It is well known that the validity of the so called Lenard-Magri scheme of integrability of a bi-Hamiltonian PDE can be established if one has some precise information on the corresponding 1st variational Poisson cohomology for one of the…

Mathematical Physics · Physics 2015-12-18 Alberto De Sole , Victor G. Kac

Generalizing a construction of P. Vanhaecke, we introduce a large class of degenerate (i.e., associated to a degenerate Poisson bracket) completely integrable systems on (a dense subset of) the space $\R^{2d+n+1}$, called the generalized…

solv-int · Physics 2008-02-03 Peter Bueken

We obtain the full hamiltonian structure for a parametric coupled KdV system. The coupled system arises from four different real basic lagrangians. The associated hamiltonian functionals and the corresponding Poisson structures follow from…

Mathematical Physics · Physics 2014-09-09 A. Restuccia , A. Sotomayor

We construct integrable Hamiltonian systems such that functionally independent Poisson commuting integrals are quadratic in the momenta. Unlike the classical St\"ackel setting, we allow the associated self-adjoint $(1,1)$-tensors $K_\alpha$…

Exactly Solvable and Integrable Systems · Physics 2025-12-22 Alexey V. Bolsinov , Andrey Yu. Konyaev , Vladimir S. Matveev

Kahan discretization is applicable to any quadratic vector field and produces a birational map which approximates the shift along the phase flow. For a planar quadratic Hamiltonian vector field with a linear Poisson tensor and with a…

Exactly Solvable and Integrable Systems · Physics 2023-03-29 Matteo Petrera , Yuri B. Suris

The Eisenhart geometric formalism, which transforms an Euclidean natural Hamiltonian $H=T+V$ into a geodesic Hamiltonian ${\cal T}$ with one additional degree of freedom, is applied to the four families of quadratically superintegrable…

Mathematical Physics · Physics 2017-02-09 Jose F. Cariñena , Francisco J. Herranz , Manuel F. Rañada

The reduction by restricting the spectral parameters $k$ and $k'$ on a generic algebraic curve of degree $\mathcal{N}$ is performed for the discrete AKP, BKP and CKP equations, respectively. A variety of two-dimensional discrete integrable…

Exactly Solvable and Integrable Systems · Physics 2017-11-27 Wei Fu , Frank Nijhoff

Given a compact symplectic toric manifold $(M,\omega, \mathbb{T})$, we identify a class $DGK_{\omega}^{\mathbb{T}}(M)$ of $\mathbb{T}$-invariant generalized K\"ahler structures for which a generalisation the Abreu-Guillemin theory of toric…

Differential Geometry · Mathematics 2015-09-28 Laurence Boulanger

We propose a systematic procedure called the Clebsch canonization for obtaining a canonical Hamiltonian system that is related to a given Lie-Poisson equation via a momentum map. We describe both coordinate and geometric versions of the…

Mathematical Physics · Physics 2023-03-24 Buddhika Jayawardana , Philip J. Morrison , Tomoki Ohsawa

Some new Hamiltonian systems of quasi-Painlev\'e type are presented and the analogue of Okamoto's space of initial conditions computed. Using the geometric approach that was introduced originally for the identification problem of Painlev\'e…

Classical Analysis and ODEs · Mathematics 2025-12-10 Marta Dell'Atti , Thomas Kecker

The $r$-KdV-CH hierarchy is a generalization of the Korteweg-de Vries and Camassa-Holm hierarchies parametrized by $r+1$ constants. In this paper we clarify some properties of its multi-Hamiltonian structures, prove the semisimplicity of…

Exactly Solvable and Integrable Systems · Physics 2008-09-03 Ming Chen , Si-Qi Liu , Youjin Zhang

We perform variable separation in the quasi-potential systems of equations of the form $\ddot{q}=-A^{-1}\nabla k=-\tilde{A}^{-1}\nabla\tilde{k}${}, where $A$ and $\tilde{A}$ are Killing tensors, by embedding these systems into a…

Exactly Solvable and Integrable Systems · Physics 2009-11-07 Krzysztof Marciniak , Maciej Blaszak