Abstract

The spin-\frac{1}{2}12 Heisenberg XXZ chain is a paradigmatic quantum integrable model. Although it can be solved exactly via Bethe ansatz techniques, there are still open issues regarding the spectrum at root of unity values of the anisotropy. We construct Baxter’s Q operator at arbitrary anisotropy from a two-parameter transfer matrix associated to a complex-spin auxiliary space. A decomposition of this transfer matrix provides a simple proof of the transfer matrix fusion and Wronskian relations. At root of unity a truncation allows us to construct the Q operator explicitly in terms of finite-dimensional matrices. From its decomposition we derive truncated fusion and Wronskian relations as well as an interpolation-type formula that has been conjectured previously. We elucidate the Fabricius–McCoy (FM) strings and exponential degeneracies in the spectrum of the six-vertex transfer matrix at root of unity. Using a semicyclic auxiliary representation we give a conjecture for creation and annihilation operators of FM strings for all roots of unity. We connect our findings with the `string-charge duality’ in the thermodynamic limit, leading to a conjecture for the imaginary part of the FM string centres with potential applications to out-of-equilibrium physics.

Highlights

  • In this work we focus on the homogeneous XXZ spin chain

  • We focus on the spin-chain perspective, note that these phenomena are relevant for the root-of-unity case of the six-vertex model, whose transfer matrix gives rise to the XXZ Hamiltonian (2.1), see Section 3

  • If N is odd the XXZ spin chain is still invariant under a global spin flip, reversing ↑ ↔ ↓ everywhere, but there are no infinite roots and we have not been able to find a simple relation between the Bethe roots {vm }mM =1 and {um}mM=1 on the two sides of the equator

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Summary

Introduction

To study the dynamics of a quantum many-body system, it is of vital importance to know the full spectrum, i.e. all eigenstates of the Hamiltonian. Using quantum integrability [9, 10] it is possible to obtain the spectrum For these models, the transfer matrices are the generating functions of the conserved (quasi-)local charges that contribute to the dynamics in the thermodynamic limit. The eigenvalues of the transfer matrix are obtained via a set of rapidity parameters whose physical values, called Bethe roots, obey the Bethe equations [13] The latter follow in a straightforward way from a difference equation known as Baxter’s TQ relation [9, 14,15,16].

XXZ spin chain
Bethe roots at infinity
Fabricius–McCoy strings
Basics of the QISM
Transfer matrices
Factorisation of Ths w
Matrix TQ relation and transfer matrix fusion relation
Truncated transfer matrix at root of unity
Applications to XXZ at root of unity: general results
Applications to XXZ at root of unity: examples
Conjectures for FM creation and annihilation operators
10 Thermodynamic limit
11 Conclusion

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