Abstract

We analyze the relaxation to equilibrium for kinetically constrained spin models (KCSM) when the initial distribution νν is different from the reversible one, μμ. This setting has been intensively studied in the physics literature to analyze the slow dynamics which follows a sudden quench from the liquid to the glass phase. We concentrate on two basic oriented KCSM: the East model on $\bbZ$, for which the constraint requires that the East neighbor of the to-be-update vertex is vacant and the model on the binary tree introduced in \cite{Aldous:2002p1074}, for which the constraint requires the two children to be vacant. While the former model is ergodic at any p≠1p\neq 1, the latter displays an ergodicity breaking transition at pc=1/2p_c=1/2. For the East we prove exponential convergence to equilibrium with rate depending on the spectral gap if νν is concentrated on any configuration which does not contain a forever blocked site or if νν is a Bernoulli(p′p') product measure for any p′≠1p'\neq 1. For the model on the binary tree we prove similar results in the regime p,p′<pcp,p'<p_c and under the (plausible) assumption that the spectral gap is positive for p<pcp<p_c. By constructing a proper test function we also prove that if p′>pcp'>p_c and p≤pcp\leq p_c convergence to equilibrium cannot occur for all local functions. Finally we present a very simple argument (different from the one in \cite{Aldous:2002p1074}) based on a combination of combinatorial results and ``energy barrier'' considerations, which yields the sharp upper bound for the spectral gap of East when p↑1p\uparrow 1.

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