Classical integrable systems and soliton equations related to eleven-vertex R-matrix
In our recent paper we suggested a natural construction of the classical relativistic integrable tops in terms of the quantum R-matrices. Here we study the simplest case – the 11-vertex R-matrix and related gl2 rational models. The corresponding top is equivalent to the 2-body Ruijsenaars–Schneider...
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doaj-b9447f43252042609ce9b8caab4dfda52020-11-24T22:24:17ZengElsevierNuclear Physics B0550-32131873-15622014-10-01887C40042210.1016/j.nuclphysb.2014.09.001Classical integrable systems and soliton equations related to eleven-vertex R-matrixA. Levin0M. Olshanetsky1A. Zotov2NRU HSE, Department of Mathematics, Myasnitskaya str. 20, Moscow, 101000, RussiaITEP, B. Cheremushkinskaya str. 25, Moscow, 117218, RussiaSteklov Mathematical Institute RAS, Gubkina str. 8, Moscow, 119991, RussiaIn our recent paper we suggested a natural construction of the classical relativistic integrable tops in terms of the quantum R-matrices. Here we study the simplest case – the 11-vertex R-matrix and related gl2 rational models. The corresponding top is equivalent to the 2-body Ruijsenaars–Schneider (RS) or the 2-body Calogero–Moser (CM) model depending on its description. We give different descriptions of the integrable tops and use them as building blocks for construction of more complicated integrable systems such as Gaudin models and classical spin chains (periodic and with boundaries). The known relation between the top and CM (or RS) models allows to rewrite the Gaudin models (or the spin chains) in the canonical variables. Then they assume the form of n-particle integrable systems with 2n constants. We also describe the generalization of the top to 1+1 field theories. It allows us to get the Landau–Lifshitz type equation. The latter can be treated as non-trivial deformation of the classical continuous Heisenberg model. In a similar way the deformation of the principal chiral model is described.http://www.sciencedirect.com/science/article/pii/S0550321314002703 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
A. Levin M. Olshanetsky A. Zotov |
spellingShingle |
A. Levin M. Olshanetsky A. Zotov Classical integrable systems and soliton equations related to eleven-vertex R-matrix Nuclear Physics B |
author_facet |
A. Levin M. Olshanetsky A. Zotov |
author_sort |
A. Levin |
title |
Classical integrable systems and soliton equations related to eleven-vertex R-matrix |
title_short |
Classical integrable systems and soliton equations related to eleven-vertex R-matrix |
title_full |
Classical integrable systems and soliton equations related to eleven-vertex R-matrix |
title_fullStr |
Classical integrable systems and soliton equations related to eleven-vertex R-matrix |
title_full_unstemmed |
Classical integrable systems and soliton equations related to eleven-vertex R-matrix |
title_sort |
classical integrable systems and soliton equations related to eleven-vertex r-matrix |
publisher |
Elsevier |
series |
Nuclear Physics B |
issn |
0550-3213 1873-1562 |
publishDate |
2014-10-01 |
description |
In our recent paper we suggested a natural construction of the classical relativistic integrable tops in terms of the quantum R-matrices. Here we study the simplest case – the 11-vertex R-matrix and related gl2 rational models. The corresponding top is equivalent to the 2-body Ruijsenaars–Schneider (RS) or the 2-body Calogero–Moser (CM) model depending on its description. We give different descriptions of the integrable tops and use them as building blocks for construction of more complicated integrable systems such as Gaudin models and classical spin chains (periodic and with boundaries). The known relation between the top and CM (or RS) models allows to rewrite the Gaudin models (or the spin chains) in the canonical variables. Then they assume the form of n-particle integrable systems with 2n constants. We also describe the generalization of the top to 1+1 field theories. It allows us to get the Landau–Lifshitz type equation. The latter can be treated as non-trivial deformation of the classical continuous Heisenberg model. In a similar way the deformation of the principal chiral model is described. |
url |
http://www.sciencedirect.com/science/article/pii/S0550321314002703 |
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