Quantum Group Theory in $\tau^{(2)}$-model, Duality of $\tau^{(2)}$-model and XXZ-model with Cyclic ${\bf U_q(sl_2)}$-representation for ${\bf q^n =1}$, and Chiral Potts Model

TL;DR

This paper explores the quantum group structure within the $ au^{(2)}$-model, establishes dualities with the XXZ-model at roots of unity, and connects these to the chiral Potts model through transfer matrices and $Q$-operators.

Contribution

It identifies the quantum group ${ extsl{U}}_ extsl{w}(sl_2)$ in the $ au^{(2)}$-model, analyzes the eigenstructure of XXZ-models with cyclic representations, and establishes dualities and connections to the chiral Potts model.

Findings

Eigenvalues and eigenvectors of XXZ-model determined by $ au^{(2)}$-model.

Identification of $Q$-operator with chiral Potts transfer matrices.

Duality between $ au^{(2)}$-models and XXZ-models at roots of unity.

Abstract

We identify the quantum group ${\Large\textsl{U}}_\textsl{w}(sl_2)$ in the $L$-operator of $\tau^{(2)}$-model for a generic $\textsl{w}$ as a subalgebra of $U_{\sf q} (sl_2)$ with $\textsl{w} = {\sf q}^{-2}$. In the roots of unity case, ${\sf q}=q, \textsl{w} = \omega$ with $q^{{\bf n}} = \omega^N = 1$, the eigenvalues and eigenvectors of XXZ-model with the $U_q (sl_2)$-cyclic representation are determined by the $\tau^{(2)}$-model with the induced ${\Large\textsl{U}}_\omega(sl_2)$-cyclic representation, which is decomposed as a finite sum of $\tau^{(2)}$-models in non-superintegrable inhomogeneous $N$-state chiral Potts model. Through the theory of chiral Potts model, the $Q$-operator of XXZ-model can be identified with the related chiral Potts transfer matrices, with special features appeared in the ${\bf n}=2N$, e.g. $N$ even, case. We also establish the duality of $\tau^{(2)}$-models related to cyclic representations of $U_q (sl_2)$, analogous to the $\tau^{(2)}$-duality in chiral Potts model; and identify the model dual to the XXZ model with $U_q (sl_2)$-cyclic representation.