Continuous eigenfunctions of the transfer operator for Dyson models
Anders Johansson, Anders Öberg, Mark Pollicott
TL;DR
This work proves the existence of a continuous eigenfunction for the transfer operator associated with long-range Dyson-type potentials under subcritical temperatures and square-summable variations of the one-point potential. The authors deploy a FK-Ising/random-cluster representation, casting the eigenfunction as a Radon-Nikodym derivative between two Gibbs measures and proving uniform convergence of finite-n likelihood ratios via percolation tail bounds. As a key corollary, they establish the existence of a continuous eigenfunction for Dyson potentials J(k)=β k^{-α} in the subcritical regime for α>3/2, thereby extending regularity results beyond summable variation. The results connect Gibbsian structure, g-measures/Doeblin theory, and percolation phenomena in long-range Ising models, with potential implications for statistical mechanics and ergodic theory of infinite-range systems.
Abstract
In this article we address a well known problem at the intersection of ergodic theory and statistical mechanics. We prove that there exists a continuous eigenfunction for the transfer operator corresponding to pair potentials that satisfy a square summability condition on the variations, when the inverse temperature is subcritical. As a corollary we obtain a continuous eigenfunction for the classical Dyson model, with interactions $\J(k)=β\, k^{-α}$, $k\ge1$, in the whole subcritical regime $β<β_c$ for which the parameter $α$ is greater than $3/2$.
