paper

Mean Field Behavior during the Big Bang Regime for Coalescing Random Walks

arXiv:2105.11585 · doi:10.1214/22-AOP1571

Abstract

In this paper we consider coalescing random walks on a general connected graph . We set up a unified framework to study the leading order of the decay rate of , the expectation of the fraction of occupied sites at time , particularly for the `Big Bang' regime where . Our results show that satisfies certain mean field behavior, if the graphs satisfy certain transience-like conditions. We apply this framework to two families of graphs: (1) graphs given by the configuration model with a degree distribution supported in for some , and (2) finite and infinite vertex-transitive graphs. In the first case, we show that for , decays in the order of , and is approximately the probability that two particles starting from the root of the corresponding unimodular Galton-Watson tree never collide after one of them leaves the root, which is also roughly , where is the mean meeting time of two walkers. By taking the local weak limit, for the unimodular Galton-Watson tree we prove the convergence of as . For the second family of graphs, if we take a sequence of finite graphs , such that and the inverse of the spectral gap is , then for , is approximately the probability that two random walks never meet before time , and also . In addition, we define a natural uniform transience condition, and show that it implies the above for all . Such estimates of are also obtained for all infinite transient transitive unimodular graphs, in particular, all transient transitive amenable graphs.

72 pages

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