Abstract

We consider random walks over polymer chains (modeled as simple random walks or self-avoiding walks) and allow from each polymer site jumps to all Euclidean (not necessarily chemical) neighboring sites. For frozen chain configurations the distribution of displacements (DD) of a walker along the chain shows a paradoxal behavior: The DD's width (interquartile distance) grows with time as $\ensuremath{\Lambda}\ensuremath{\propto}{t}^{\ensuremath{\alpha}}$, with $\ensuremath{\alpha}\ensuremath{\approx}0.5$, but the DD displays large power-law tails. For annealed configurations the DD is a L\'evy distribution and its width is strongly superdiffusive.

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