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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Main Authors: A. Levin, M. Olshanetsky, A. Zotov
Format: Article
Language:English
Published: Elsevier 2014-10-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321314002703
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spelling 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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AT molshanetsky classicalintegrablesystemsandsolitonequationsrelatedtoelevenvertexrmatrix
AT azotov classicalintegrablesystemsandsolitonequationsrelatedtoelevenvertexrmatrix
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