4.4 Article

Relativistic classical integrable tops and quantum R-matrices

Journal

JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 7, Pages -

Publisher

SPRINGER
DOI: 10.1007/JHEP07(2014)012

Keywords

Integrable Equations in Physics; Quantum Groups; Gauge Symmetry

Funding

  1. RFBR [12-02-00594, 12-01-00482]
  2. AG Laboratory GU-HSE, RF government [11 11.G34.31.0023]
  3. D. Zimin's fund Dynasty
  4. Program of RAS Basic Problems of the Nonlinear Dynamics in Mathematical and Physical Sciences
  5. RFBR [12-02-00594, 12-01-00482]
  6. AG Laboratory GU-HSE, RF government [11 11.G34.31.0023]
  7. D. Zimin's fund Dynasty
  8. Program of RAS Basic Problems of the Nonlinear Dynamics in Mathematical and Physical Sciences

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We describe classical top-like integrable systems arising from the quantum exchange relations and corresponding Sklyanin algebras. The Lax operator is expressed in terms of the quantum non-dynamical R-matrix even at the classical level, where the Planck constant plays the role of the relativistic deformation parameter in the sense of Ruijsenaars and Schneider (RS). The integrable systems (relativistic tops) are described as multidimensional Euler tops, and the inertia tensors are written in terms of the quantum and classical R-matrices. A particular case of gl(N) system is gauge equivalent to the N-particle RS model while a generic top is related to the spin generalization of the RS model. The simple relation between quantum R-matrices and classical Lax operators is exploited in two ways. In the elliptic case we use the Belavin's quantum R-matrix to describe the relativistic classical tops. Also by the passage to the noncommutative torus we study the large N limit corresponding to the relativistic version of the nonlocal 2d elliptic hydrodynamics. Conversely, in the rational case we obtain a new glN quantum rational non-dynamical R-matrix via the relativistic top, which we get in a different way using the factorized form of the RS Lax operator and the classical Symplectic Hecke (gauge) transformation. In particular case of gl(2) the quantum rational R-matrix is 11-vertex. It was previously found by Cherednik. At last, we describe the integrable spin chains and Gaudin models related to the obtained R-matrix.

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