Freezing phase transition for the Thue-Morse subshift
Nicolas Bédaride, Julien Cassaigne, Pascal Hubert, Renaud Leplaideur
TL;DR
This work analyzes the pressure for a non-Hölder prefix-based potential defined via the Thue-Morse subshift on the full two-symbol shift and proves a freezing phase transition: for sufficiently large β, the pressure collapses to 0 and the unique equilibrium state is the TM-invariant measure with zero entropy. The authors deploy an inducing scheme on a cylinder outside TM and a transfer operator L_{z,β,V}, reducing the problem to bounding sums over return words and accident words encoded by a carefully constructed infinite matrix. They establish finiteness and convergence of these sums for β>4 and provide explicit, though non-optimal, bounds (β0<16.6 for a canonical V0) showing the phase transition, with a method to extend to a broad class of potentials Ξ. The results clarify freezing phenomena for substitution subshifts, address gaps in prior proofs, and offer an algorithmic approach for analyzing other substitutions, contributing to understanding quasicrystal-like symbolic systems within thermodynamic formalism.
Abstract
On the full shift on two symbols, we consider the potential defined by $V(x) = \frac{1}{n}$ where $n$ denotes the longest common prefix between the infinite word $x$ and an element of the subshift associated to the Thue-Morse substitution. Given a non negative real number $β$, the pressure function is $P(β):=\sup\left\{h_μ+β\int V\,dμ\right\},$ where the supremum is taken over all shift invariant probabilities $μ$ on the full shift and $h_μ$ is the Kolmogorov entropy. We prove that there is a freezing phase transition for the potential $V$: For $β$ large enough, the pressure $P(\be)$ is equal to zero. Similar results were previously published by Bruin and Leplaideur in \cite{BL2}, \cite{Bruin-Leplaid-13} but their proofs contained significant gaps and required substantial clarification.
