Clusters in the critical branching Brownian motion
arXiv:2209.10822 · doi:10.1088/1751-8121/acbb46
Abstract
Brownian particles that are replicated and annihilated at equal rate have strongly correlated positions, forming a few compact clusters separated by large gaps. We characterize the distribution of the particles at a given time, using a definition of clusters in terms a coarse-graining length recently introduced by some of us. We show that, in a non-extinct realization, the average number of clusters grows as where is the Haussdoff dimension of the boundary of the super-Brownian motion, found by Mueller, Mytnik, and Perkins. We also compute the distribution of gaps between consecutive particles. We find two regimes separated by the characteristic length scale where is the diffusion constant and the branching rate. The average number of gaps greater than decays as for and for . Finally, conditioned on the number of particles , the above distributions are valid for ; the average number of gaps greater than is much less than one, and decays as , in agreement with the universal gap distribution predicted by Ramola, Majumdar, and Schehr. Our results interpolate between a dense super-Brownian motion regime and a large-gap regime, unifying two previously independent approaches.
20 pages, 9 figure; v2, minor revisions, accepted version
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