The mixing time evolution of Glauber dynamics for the mean-field Ising model

TL;DR

This paper characterizes how the mixing time of Glauber dynamics for the mean-field Ising model transitions from high to low temperature regimes as the temperature approaches the critical point, revealing detailed scaling behaviors.

Contribution

It provides a complete description of the mixing time behavior near the critical temperature, including cutoff phenomena and precise scaling laws as the temperature varies with system size.

Findings

Mixing time in high temperature regime is order (n/δ) log(δ^2 n).

At the critical window, mixing time is order n^{3/2} with no cutoff.

Below the critical temperature, mixing time grows exponentially with δ^2 n.

Abstract

We consider Glauber dynamics for the Ising model on the complete graph on $n$ vertices, known as the Curie-Weiss model. It is well-known that the mixing-time in the high temperature regime ($\beta < 1$) has order $n\log n$, whereas the mixing-time in the case $\beta > 1$ is exponential in $n$. Recently, Levin, Luczak and Peres proved that for any fixed $\beta < 1$ there is cutoff at time $[2(1-\beta)]^{-1} n\log n$ with a window of order $n$, whereas the mixing-time at the critical temperature $\beta=1$ is $\Theta(n^{3/2})$. It is natural to ask how the mixing-time transitions from $\Theta(n\log n)$ to $\Theta(n^{3/2})$ and finally to $\exp(\Theta(n))$. That is, how does the mixing-time behave when $\beta=\beta(n)$ is allowed to tend to 1 as $n\to\infty$. In this work, we obtain a complete characterization of the mixing-time of the dynamics as a function of the temperature, as it approaches its critical point $\beta_c=1$. In particular, we find a scaling window of order $1/\sqrt{n}$ around the critical temperature. In the high temperature regime, $\beta = 1 - \delta$ for some $0 < \delta < 1$ so that $\delta^2 n \to\infty$ with $n$, the mixing-time has order $(n/\delta)\log(\delta^2 n)$, and exhibits cutoff with constant 1/2 and window size $n/\delta$. In the critical window, $\beta = 1\pm \delta$ where $\delta^2 n$ is O(1), there is no cutoff, and the mixing-time has order $n^{3/2}$. At low temperature, $\beta = 1 + \delta$ for $\delta > 0$ with $\delta^2 n \to\infty$ and $\delta=o(1)$, there is no cutoff, and the mixing time has order $(n/\delta)\exp(({3/4}+o(1))\delta^2 n)$.