Fourth-neighbour two-point functions of the XXZ chain and the Fermionic basis approach

TL;DR

This paper reviews the Fermionic basis approach to calculating correlation functions in the XXZ quantum spin chain, providing explicit formulas suitable for computer implementation and analyzing fourth-neighbour two-point functions.

Contribution

It introduces explicit, algebraic formulas for short-range correlation functions in the XXZ chain using the Fermionic basis, applicable to various ensembles and regimes.

Findings

Explicit formulas for four-neighbour two-point functions

Comparison with asymptotic results at zero and finite temperature

Factorized form of stationary reduced density matrices

Abstract

We give a descriptive review of the Fermionic basis approach to the theory of correlation functions of the XXZ quantum spin chain. The emphasis is on explicit formulae for short-range correlation functions which will be presented in a way that allows for their direct implementation on a computer. Within the Fermionic basis approach a huge class of stationary reduced density matrices, compatible with the integrable structure of the model, assumes a factorized form. This means that all expectation values of local operators and all two-point functions, in particular, can be represented as multivariate polynomials in only two functions $\rho$ and $\omega$ and their derivatives with coefficients that are rational in the deformation parameter $q$ of the model. These coefficients are of `algebraic origin'. They do not depend on the choice of the density matrix, which only impacts the form of $\rho$ and $\omega$. As an example we work out in detail the case of the grand canonical ensemble at temperature $T$ and magnetic field $h$ for $q$ in the critical regime. We compare our exact results for the fourth-neighbour two-point functions with asymptotic formulae for $h, T = 0$ and for finite $h$ and $T$.