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Quantum deformations of the one-dimensional Hubbard model

Niklas Beisert1 and Peter Koroteev1,2,3

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The centrally extended superalgebra \alg{psu}(2|2) \ltimes{\bb R}^3 was shown to play an important role for the integrable structures of the one-dimensional Hubbard model and of the planar AdS/CFT correspondence. Here we consider its quantum deformation {\rm U}_q(\alg{psu}(2|2) \ltimes{\bb R}^3) and derive the fundamental R-matrix. From the latter we deduce an integrable spin-chain Hamiltonian with three independent parameters and the corresponding Bethe equations to describe the spectrum on periodic chains. We relate our Hamiltonian to a two-parametric Hamiltonian proposed by Alcaraz and Bariev which can be considered a quantum deformation of the one-dimensional Hubbard model.


PACS

75.10.Lp Band and itinerant models

75.10.Dg Crystal-field theory and spin Hamiltonians

75.10.Jm Quantized spin models

MSC

81R50 Quantum groups and related algebraic methods (See also 16W35, 17B37)

17B37 Quantum groups (quantized enveloping algebras) and related deformations (See also 16W35, 20G42, 81R50, 82B23)

Subjects

Condensed matter: electrical, magnetic and optical

Dates

Issue 25 (27 June 2008)

Received 3 April 2008

Published 28 May 2008



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