We study diffusion of Brownian particles on random fractal structures, self‐avoiding random walks and percolation clusters at criticality, which serve as model systems for polymers in a good solvent and random two‐component mixtures, respectively. Using numerical simulations and scaling arguments we find that the distribution function P ( r, t ) of the particles is a stretched Gaussian and scales as log[ P ( r, t )/ P ( r , 0)] ∼ —[ r/R ( t )] u , where R ( t ) ∼ t 1/dw is the root‐mean‐square displacement, u = d w /( d w ‐1), and d w = 2 d f for self‐avoiding walks and d w = 3 d f /2 for percolation; d f is the fractal dimension of the structure. In the presence of an external constant bias field, diffusion is drastically reduced and R ( t ) ∼ log t evolves logarithmically in time, in exactly the same way in both fractal structures.
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Roman et al. (1989) studied this question.
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