Abstract
Critical correlation in thermal systems, Ising spins for example, is approximately described by clusters. A cluster is defined as a randomly picked, connected region of excess up (or down) spins. Its simulation utilizes a branching-out stochastic chain which allots spins continuously, either to the cluster or to a perimeter of average composition. Results in dimensionality from 2 to 10 show the cluster geometry to be very different than in (athermal) percolation.

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