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arXiv:cond-mat/9911043 · Journal of Physics A Mathematical and General

Exactly solvable quantum spin ladders associated with the orthogonal and symplectic Lie algebras

Murray T. Batchelor, Jan de Gier, Jon Links, M. Maslen

Published Mar 23, 2000• 25 citations
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Abstract

We extend the results of spin ladder models associated with the Lie algebras su (2 n ) to the case of the orthogonal and symplectic algebras o (2 n ), sp (2 n ) where n is the number of legs for the system. Two classes of models are found whose symmetry, either orthogonal or symplectic, has an explicit n dependence. Integrability of these models is shown for an arbitrary coupling of XX -type rung interactions and applied magnetic field term.

DOI
10.1088/0305-4470/33/12/101

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We extend the results of spin ladder models associated with the Lie algebras su (2 n ) to the case of the orthogonal and symplectic algebras o (2 n ), sp (2 n ) where n is the number of legs for the system. Two classes of models are found whose symmetry, either orthogonal or symplectic, has an explicit n dependence. Integrability of these models is shown for an arbitrary coupling of XX -type rung interactions and applied magnetic field term.
Two integrable quantum spin ladder systems will be introduced associated with the fundamental su(2|2) solution of the Yang-Baxter equation. The first model is a generalized quantum Ising system with Ising rung interactions. In the second model the addition of extra interactions allows us to impose Heisenberg rung interactions without violating integrability. The existence of a Bethe ansatz solution for both models allows us to investigate the elementary excitations for antiferromagnetic rung couplings. We find that the first model does not show a gap whilst in the second case there is a gap for all positive values of the rung coupling.
We study boundary rung defects in n-leg quantum spin ladders with SU(2n)\mathrm{SU}{(2}^{n})SU(2n) leg symmetry. The rung interactions are parametrized by two coupling parameters J and ${J}^{\ensuremath{'}}$ interpolating between the uniform spin tube ${(J}^{\ensuremath{'}}=J)$ and the open spin ladder ${(J}^{\ensuremath{'}}=0).$ The rung defect at the edge of the ladder has rung coupling parameters Jd{J}_{d}Jd​ and ${J}_{d}^{\ensuremath{'}}.$ The conditions for the integrability of the model are investigated as a function of n, J, ${J}^{\ensuremath{'}},$ Jd,{J}_{d},Jd​, and ${J}_{d}^{\ensuremath{'}},$ and the Bethe Ansatz equations for the exact solution are derived. The boundary quantum critical behavior is discussed. The conditions for the formation of a local moment (boundary bound state due to the defect) are studied. In the absence of a magnetic field such a bound state is only possible for even-legged spin tubes, while for odd-legged ladders a bound state can only occur in a large magnetic field. Depending on the parameters of the host this local moment may be screened in analogy to the Kondo effect.