KMS states on Nica-Toeplitz C*-algebras

TL;DR

This paper characterizes KMS states on Nica-Toeplitz algebras associated with quasi-lattice ordered groups and product systems, establishing a bijection with tracial states and analyzing phase transitions at critical inverse temperatures.

Contribution

It generalizes existing results by removing assumptions on P and X, and provides a comprehensive framework for studying KMS states at any inverse temperature.

Findings

Bijection between gauge-invariant KMS states and tracial states on A.

Existence of a critical inverse temperature with phase transition.

Reduction of inequality systems for finitely generated monoids.

Abstract

Given a quasi-lattice ordered group $(G,P)$ and a compactly aligned product system $X$ of essential C$^*$-correspondences over the monoid $P$, we show that there is a bijection between the gauge-invariant KMS$_\beta$-states on the Nica-Toeplitz algebra $\mathcal{NT}(X)$ of $X$ with respect to a gauge-type dynamics, on one side, and the tracial states on the coefficient algebra $A$ satisfying a system (in general infinite) of inequalities, on the other. This strengthens and generalizes a number of results in the literature in several directions: we do not make any extra assumptions on $P$ and $X$, and our result can, in principle, be used to study KMS-states at any finite inverse temperature $\beta$. Under fairly general additional assumptions we show that there is a critical inverse temperature $\beta_c$ such that for $\beta>\beta_c$ all KMS$_\beta$-states are of Gibbs type, hence gauge-invariant, in which case we have a complete classification of KMS$_\beta$-states in terms of tracial states on $A$, while at $\beta=\beta_c$ we have a phase transition manifesting itself in the appearance of KMS$_\beta$-states that are not of Gibbs type. In the case of right-angled Artin monoids we show also that our system of inequalities for traces on $A$ can be reduced to a much smaller system, a finite one when the monoid is finitely generated. Most of our results generalize to arbitrary quasi-free dynamics on $\mathcal{NT}(X)$.