(3) Polynomial Integrable System: Different Faces of the 3-Body/₂ Elliptic Calogero Model

• Published in: Symmetry, Integrability and Geometry: Methods and Applications
• Date: 2024
• Main Authors: Turbiner, Alexander V., Lopez Vieyra, Juan Carlos, Guadarrama-Ayala, Miguel A.
• Format: Article
• Language: English
• Published: Інститут математики НАН України 2024
• Online Access: https://nasplib.isofts.kiev.ua/handle/123456789/212111
• Journal Title: Digital Library of Periodicals of National Academy of Sciences of Ukraine
• Cite this: (3) Polynomial Integrable System: Different Faces of the 3-Body/₂ Elliptic Calogero Model. Alexander V. Turbiner, Juan Carlos Lopez Vieyra and Miguel A. Guadarrama-Ayala. SIGMA 20 (2024), 012, 23 pages

It is shown that the (3) polynomial integrable system, introduced by Sokolov-Turbiner in [J. Phys. A 48 (2015), 155201, 15 pages, arXiv:1409.7439], is equivalent to the (3) quantum Euler-Arnold top in a constant magnetic field. Their Hamiltonian and third-order integral can be rewritten in terms of the (3) algebra generators. In turn, all these (3) generators can be represented by the non-linear elements of the universal enveloping algebra of the 5-dimensional Heisenberg algebra ₅(^₁,₂, ^₁,₂, ); thus, the Hamiltonian and integral are two elements of the universal enveloping algebra ₅. In this paper, four different representations of the ₅ Heisenberg algebra are used: (I) by differential operators in two real (complex) variables, (II) by finite-difference operators on uniform or exponential lattices. We discovered the existence of two 2-parametric bilinear and trilinear elements (denoted and , respectively) of the universal enveloping algebra ((3)) such that their Lie bracket (commutator) can be written as a linear superposition of nine so-called artifacts - the special bilinear elements of ((3)), which vanish once the representation of the (3)-algebra generators is written in terms of the ₅(^₁,₂, ^₁,₂, )-algebra generators. In this representation, all nine artifacts vanish, two of the above-mentioned elements of U((3)) (called the Hamiltonian H and the integral I) commute(!); in particular, they become the Hamiltonian and the integral of the 3-body elliptic Calogero model, if (^, ^) are written in the standard coordinate-momentum representation. If (^, ^) are represented by finite-difference/discrete operators on uniform or exponential lattices, the Hamiltonian and the integral of the 3-body elliptic Calogero model become the isospectral, finite-difference operators on uniform-uniform or exponential-exponential lattices (or mixed) with polynomial coefficients. If (^, ^) are written in complex (, ¯) variables, the Hamiltonian corresponds to a complexification of the 3-body elliptic Calogero model on ℂ².