arXiv2009
We show that the group ${\mathbb Q \rtimes \mathbb Q^*_+}$ of orientation-preserving affine transformations of the rational numbers is quasi-lattice ordered by its subsemigroup ${\mathbb N \rtimes \mathbb N^\times}$. The associated Toeplitz $C^*$-algebra ${\mathcal T}({\mathbb N \rtimes \mathbb N^\times})$ is universal for isometric representations which are covariant in the sense of Nica. We give a presentation of this Toeplitz algebra in terms of generators and relations, and use this to show that the $C^*$-algebra ${\mathcal Q_\mathbb N}$ recently introduced by Cuntz is the boundary quotient of $({\mathbb Q \rtimes \mathbb Q^*_+}, {\mathbb N \rtimes \mathbb N^\times})$ in the sense of Crisp and Laca. The Toeplitz algebra ${\mathcal T}({\mathbb N \rtimes \mathbb N^\times})$ carries a natural dynamics $σ$, which induces the one considered by Cuntz on the quotient ${\mathcal Q_\mathbb N}$, and our main result is the computation of the KMS$_β$ (equilibrium) states of the dynamical system $({\mathcal T}({\mathbb N \rtimes \mathbb N^\times}), {\mathbb R},σ)$ for all values of the inverse temperature $β$. For $β\in [1, 2]$ there is a unique KMS$_β$ state, and the KMS$_1$ state factors through the quotient map onto ${\mathcal Q_\mathbb N}$, giving the unique KMS state discovered by Cuntz. At $β=2$ there is a phase transition, and for $β>2$ the KMS$_β$ states are indexed by probability measures on the circle. There is a further phase transition at $β=\infty$, where the KMS$_\infty$ states are indexed by the probability measures on the circle, but the ground states are indexed by the states on the classical Toeplitz algebra ${\mathcal T}(\mathbb N)$.