## 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 (β < 1) has order n log n, whereas the mixing-time in the case β > 1 is exponential in n. Recently, Levin, Luczak and Peres proved that for any fixed β < 1 there is cutoff at time 1/2(1-β)^{n}log n with a window of order n, whereas the mixing-time at the critical temperature β = 1 is Θ(n ^{3/2}). It is natural to ask how the mixing-time transitions from Θ(n log n) to Θ(n ^{3/2}) and finally to exp (Θ(n)). That is, how does the mixing-time behave when β = β(n) is allowed to tend to 1 as n → ∞. 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 β _{c} = 1. In particular, we find a scaling window of order 1/√n around the critical temperature. In the high temperature regime, β = 1 - δ for some 0 < δ < 1 so that δ ^{2} n → ∞ with n, the mixing-time has order (n/δ) log(δ ^{2} n), and exhibits cutoff with constant 1/2 and window size n/δ. In the critical window, β = 1± δ, where δ ^{2} n is O(1), there is no cutoff, and the mixing-time has order n ^{3/2}. At low temperature, β = 1 + δ for δ > 0 with δ ^{2} n → ∞ and δ = o(1), there is no cutoff, and the mixing time has order n/δ exp((3/4 + o(1))δ^{2}n).

Original language | English (US) |
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Pages (from-to) | 725-764 |

Number of pages | 40 |

Journal | Communications In Mathematical Physics |

Volume | 289 |

Issue number | 2 |

DOIs | |

State | Published - Jul 2009 |

## ASJC Scopus subject areas

- Statistical and Nonlinear Physics
- Mathematical Physics