Ising model on trees and factors of IID

TL;DR

This paper constructs a factor of IID for the ferromagnetic Ising model on an infinite regular tree beyond the known uniqueness regime, using solutions to an infinite-dimensional stochastic differential equation.

Contribution

It introduces a novel method to create a factor of IID for the Ising model in the reconstruction regime via stochastic differential equations, extending previous results.

Findings

Constructed a factor of IID beyond the uniqueness regime

Used a strong solution to an infinite-dimensional SDE

Applicable for ng eta (d-1)^{-rac{1}{2}}

Abstract

We study the ferromagnetic Ising model on the infinite $d$-regular tree under the free boundary condition. This model is known to be a factor of IID in the uniqueness regime, when the inverse temperature $\beta\ge 0$ satisfies $\tanh \beta \le (d-1)^{-1}$. However, in the reconstruction regime ($\tanh \beta > (d-1)^{-\frac{1}{2}}$), it is not a factor of IID. We construct a factor of IID for the Ising model beyond the uniqueness regime via a strong solution to an infinite dimensional stochastic differential equation which partially answers a question of Lyons. The solution $\{X_t(v) \}$ of the SDE is distributed as \[ X_t(v) = t\tau_v + B_t(v), \] where $\{\tau_v \}$ is an Ising sample and $\{B_t(v) \}$ are independent Brownian motions indexed by the vertices in the tree. Our construction holds whenever $\tanh \beta \le c(d-1)^{-\frac{1}{2}}$, where $c>0$ is an absolute constant.