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Spectra of Transfer Matrices of Exactly Solvable Models with D(D3)Symmetry

Christopher S. Campbell

Published May 1, 2010• 0 citations
OpenAlex

Abstract

The Quantum Inverse Scattering Method, formalised in the late 70s by Faddeev, Sklyanin and Takhtadzhyan, is a method for constructing integrable quantum systems given a solution to the Yang-Baxter equation. Once constructed it is often possible to find the energy spectrum of the associated hamiltonian using the method of mutually commuting transfer matrices, and the algebraic Bethe ansatz. If the algebraic Bethe ansatz fails we are still often able to solve the system using functional relation methods. In 2006 Dancer, Isaac and Links found several solutions to the Yang-Baxter equation arising from the Drinfeld double of the dihedral group $D(D_3)$. The associated hamiltonian describes a system of interacting, non-abelian anyons. In this dissertation we take these solutions to the Yang-Baxter equation and, using a combination of algebraic Bethe ansatz and functional relations, we find the eigenvalues of the anyonic hamiltonian. The solution we find is dependent on two distinct sets of solutions to the Bethe equations, something that is rather uncommon, though not unprecedented. Further results are also obtained for other integrable models arising from the same set of solutions to the Yang-Baxter equation.

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The Quantum Inverse Scattering Method, formalised in the late 70s by Faddeev, Sklyanin and Takhtadzhyan, is a method for constructing integrable quantum systems given a solution to the Yang-Baxter equation. Once constructed it is often possible to find the energy spectrum of the associated hamiltonian using the method of mutually commuting transfer matrices, and the algebraic Bethe ansatz. If the algebraic Bethe ansatz fails we are still often able to solve the system using functional relation methods. In 2006 Dancer, Isaac and Links found several solutions to the Yang-Baxter equation arising from the Drinfeld double of the dihedral group D(D3)D(D_3)D(D3​). The associated hamiltonian describes a system of interacting, non-abelian anyons. In this dissertation we take these solutions to the Yang-Baxter equation and, using a combination of algebraic Bethe ansatz and functional relations, we find the eigenvalues of the anyonic hamiltonian. The solution we find is dependent on two distinct sets of solutions to the Bethe equations, something that is rather uncommon, though not unprecedented. Further results are also obtained for other integrable models arising from the same set of solutions to the Yang-Baxter equation.
A little over 20 years ago Drinfeld presented the quantum (or Drinfeld) double construction. This construction takes any Hopf algebra and embeds it in a larger quasi-triangular Hopf algebra, which contains an algebraic solution to the constant Yang–Baxter equation. One such class of algebras consists of the Drinfeld doubles of finite groups, which are currently of interest due to their connections with non-Abelian anyons. The smallest non-commutative Drinfeld double of a finite group algebra is the Drinfeld double of D3 , the dihedral group of order six, which was recently used to construct solutions to the Yang–Baxter equation cor- responding to 2-state and 3-state integrable spin chains with periodic boundary conditions. In this thesis we construct R-matrices from the Drinfeld double of dihedral group algebras, D(Dn) and consider their associated integrable systems. The 3-state spin chain from D(D3) is generalised to include open boundaries and it is also shown that there exists a more general R-matrix for this algebra. For general D(Dn) an R-matrix is constructed as a descendant of the zero-field six-vertex model.
Subject of this work are integrable spin chains with general boundary conditions.In the framework of the Quantum Inverse Scattering Method Sklyanin has shown how to construct a family of commuting operators (transfer matrix) containing the hamiltonian of the XXX or XXZ spin chain with general boundary fields.Key ingredient is the underlying algebraic structure which is a combination of the Yang-Baxter algebra, using the known R-matrix representations, and a so-called Reflection algebra.The latter includes fields of arbitrary strength and direction acting on the first and last position of the chain.This setup is solvable via algebraic Bethe ansatz in the case of diagonal boundaries, i.e. the fields are parallel to each other and in the case of the XXZ model parallel to the distinguished direction.Kitanine et al. have managed to express local operators in terms of the non-local elements of the underlying algebraic structure in the case of half-infinite chain length hence establishing a possible approach to evaluate expectation values of physical observables.Their results will be picked up in this work and generalized to spin chains of arbitrary (including finite) lengths using non-linear integral equations for the lowest lying state with zero magnetization.In the case of non-diagonal boundary fields the lack of a reference state or pseudo vacuum prohibits the solution by algebraic Bethe ansatz.The method of separation of variables proposed by Sklyanin is not constrained in that sense and will be applied to this situation.In this approach for the XXX spin chain no restrictions to the boundary parameters are needed.The result is a TQ-equation on a finite discrete set of points and the eigenvalues of the transfer matrix are obtainable from this finite difference equation.As the underlying algebraic structure is independent of the representation, the analysis for the XXX spin chain can be extended to a spin-boson model.Using a known representation of the algebra for the bosonic degree of freedom again a TQ-equation is obtained but in this case being defined on an infinite discrete set of points.Finally a different approach to the case of non-diagonal boundary conditions using non-linear integral equations is studied.By construction of higher dimensional representations of the Yang Baxter algebra a hierarchy of transfer matrices is obtained.In this construction two R-matrices are fused together yielding the name of fusion hierarchy.From such hierarchies it is possible to derive non-linear integral equations for a certain eigenvalue of the transfer matrix using Fourier transform techniques.The equations are valid for arbitrary system sizes and a range of boundary parameters.By careful analysis of the zero and pole structure it is possible to extract information about the eigenvalue of a specific state.
The solution of the Heisenberg model ( XXX -spin chain) is reviewed to define main ingredients of the quantum inverse scattering method. The spectrum and eigenfunctions are constructed by the algebraic Bethe Ansatz. A dynamical symmetry algebra is identified with a quantum group —the sl (2) Yangian. The Yang-Baxter equation and its GL ( n )-invariant solutions ( R -matrices) are discussed. Integral equations describing the Heisenberg model in the limit of an infinite chain are given. These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
Functional equations methods are a fundamental part of the theory of Exactly Solvable Models in Statistical Mechanics and they are intimately connected with Baxter's concept of commuting transfer matrices. This concept has culminated in the celebrated Yang-Baxter equation which plays a fundamental role for the construction of quantum integrable systems and also for obtaining their exact solution. Here I shall discuss a proposal that has been put forward in the past years, in which the Yang-Baxter algebra is viewed as a source of functional equations describing quantities of physical interest. For instance, this method has been successfully applied for the description of the spectrum of open spin chains, partition functions of elliptic models with domain wall boundaries and scalar product of Bethe vectors. Further applications of this method are also discussed.
Commuting transfer matrices for linear chains of interacting non-Abelian anyons from the two-dimensional irreducible representation of the dihedral group D3{D}_{3}D3​ [or, equivalently, the integer sector of the su(2)4su{(2)}_{4}su(2)4​ spin-1 chain] are constructed using the spin-anyon correspondence to a D3{D}_{3}D3​-symmetric formulation of the XXZ Heisenberg spin chain. The spectral problem is solved using discrete inversion identities satisfied by these transfer matrices and functional Bethe ansatz methods. The resulting spectrum can be related to that of the XXZ spin-1/2 Heisenberg chain with boundary conditions depending on the topological sector of the anyon chain. The properties of this model in the critical regime are studied by finite size analysis of the spectrum. In particular, points in the phase diagram where the anyon chain realizes some of the rational Z2{\mathbb{Z}}_{2}Z2​ orbifold theories are identified.
We formulate the quantum inverse scattering method for the case of anyonic grading. This provides a general framework for constructing integrable models describing interacting hard-core anyons. Through this method we reconstruct the known integrable model of hard core anyons associated with the XXX model, and as a new application we construct the anyonic t − J model. The energy spectrum for each model is derived by means of a generalization of the algebraic Bethe ansatz. The grading parameters implementing the anyonic signature give rise to sector-dependent phase factors in the Bethe ansatz equations.