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arXiv:hep-th/9307197 · Communications in Mathematical Physics

Staggered polarization of vertex models with $$U_q (\widehat{sl(}n))$$ -Symmetry

Yoshitaka Koyama

Published Aug 1, 1994• 46 citations
arXivHTMLPDF
DOI
10.1007/bf02101703

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Staggered polarization of vertex models with Uq(sl(^n))U_q (\widehat{sl(}n))Uq​(sl(​n)) -Symmetry
Staggered Polarization of Vertex Models with Uq(widehatsl(n))U_q(\\widehat{sl}(n))Uq​(widehatsl(n))-Symmetry
In this paper we give an explicit formula for level 1 vertex operators related to Uq(widehatsl(n))U_q(\\widehat{sl}(n))Uq​(widehatsl(n)) as operators on the Fock spaces. We derive also their commutation relations. As an applications we culculate the one point functions of the one-dimensional spin chain associated with the vector representation of Uq(widehatsl(n))U_q(\\widehat{sl}(n))Uq​(widehatsl(n)), thereby extending the recent work on the staggered polarization of the XXZXXZXXZ-model.
Generalization of the U\mathcal{U} U q (gl(N)) Algebra and Staggered Models
An eight-vertex model with staggered (site-dependent) vertex weights is considered. The model is an extension of the usual one with translationally invariant weights and contains sixteen independent vertex weights. From its Ising representation it is seen that there are actually only eleven independent parameters. After discussing some general symmetry properties of this model, we consider in detail the soluble case of a free-fermion model. We find that the staggered free-fermion model may exhibit up to three phase transitions. Generally the specific heat has logarithmic singularities, expect in some special cases it has an exponent $\ensuremath{\alpha}=\frac{1}{2}$ and the system is frozen below a unique transition point. Conditions for these special cases are given.