Analytic arguments are presented, concerning the ``phase transition'' to nonmultifractal behavior of the qth moment, Mq, of growth probabilities in diffusion-limited aggregation, found numerically by Lee and Stanley. Assuming the existence of exponentially small growth probabilities, for a single growing aggregate, we find a transition at q=0. For aggregates of size L, this transition splits into two at q₀(L)qc(L)0. Quantitative analysis of q₀(L) yields information on the tail of the growth probability distribution. Averaging Mq over all aggregates may yield a finite q₀.
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Blumenfeld et al. (1989) studied this question.
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