Abstract

For diffusive motion in random media it is widely believed that the velocity autocorrelation function c(t) exhibits power law decay as time t ..-->.. infinity. We demonstrate that the decay of c(t) in quasiperiodic media can be arbitrarily slow within the class of integrable functions. For example, in d = 1 with a potential V(x) = cos x + cos kx, there is a dense set of irrational k's such that the decay of c(k, t) is slower than 1/t/sup (1+epsilon/)/ for any epsilon > 0. The irrationals producing such a slow decay of c(k, t) are very well approximated by rationals.

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