Abstract

We study analytically and numerically the mean probability density 〈 P(r, t)〉 N of random walks on random fractals, averaged over N configurations. We find that for large distances r, 〈 P(r, t)〉 N is characterized by a crossover at r r 2 ∼ r c ( N) 1−d min 〈 R(t)〉, where 〈 R(t)〉 ∼ t 1/ d w is the r.m.s. displacement of the random walker, d min is the fractal dimension of the shortest path on the fractal and r c ( N) increases logarithmically with N. For r below r 2, In 〈 P(r,t)〉 N ∼ − a p ( r〈 R(t)〉) u does not depend on N and is characterized by the exponent u = d w /( d w − 1), while for r > r 2 the coefficient a p decreases logarithmically with N and the exponent becomes u = d min d w /( d w − d min). We discuss the relevance of the results to the important problem of localization of vibrational excitations on random fractal structures.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call