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Invited talk at

Integrable higher spin chains with SU-q(2) symmetry

Luca Mezincescu, Rafael I. Nepomechie

Published Jan 1, 1990• 0 citations
OpenAlex

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Spectral equivalences and symmetry breaking in integrableSUq(N) spin chains with boundaries

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We consider the SU q ( N ) invariant spin chain with diagonal and non-diagonal integrable boundary terms. The algebraic study of spin chains with different kinds of boundary terms is used to motivate a set of spectral equivalences between integrable chains with purely diagonal boundary terms and ones with an arbitrary non-diagonal term at one end. For each choice of diagonal boundary terms there is an iso-spectral one-boundary problem and vice versa. The cases N = 2, 3, 4 are used as examples throughout to illustrate the general structure. The quantum group SU q ( N ) symmetry is broken by the presence of a non-diagonal boundary term; however, one can use the spectral equivalence with the diagonal chain to easily understand the residual symmetries of the system. This is described in detail for the case of SU (3).

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On rational R -matrices with adjoint SU( n ) symmetry *

Laurens Stronks, Johan W. van de Leur, Dirk Schuricht

Abstract Using the representation theory of Yangians we construct the rational R -matrix which takes values in the adjoint representation of SU( n ). From this we derive an integrable SU( n ) spin chain with lattice spins transforming under the adjoint representation. However, the resulting Hamiltonian is found to be non-Hermitian.

arXiv:1606.02516•Journal of Physics A Mathematical and Theoretical•Oct 10, 2016•1 citation
We consider the SU q ( N ) invariant spin chain with diagonal and non-diagonal integrable boundary terms. The algebraic study of spin chains with different kinds of boundary terms is used to motivate a set of spectral equivalences between integrable chains with purely diagonal boundary terms and ones with an arbitrary non-diagonal term at one end. For each choice of diagonal boundary terms there is an iso-spectral one-boundary problem and vice versa. The cases N = 2, 3, 4 are used as examples throughout to illustrate the general structure. The quantum group SU q ( N ) symmetry is broken by the presence of a non-diagonal boundary term; however, one can use the spectral equivalence with the diagonal chain to easily understand the residual symmetries of the system. This is described in detail for the case of SU (3).