Abstract
Anomalous dynamics in which local perturbations spread faster than diffusion are ubiquitously observed in the long-time behavior of a wide variety of systems. Here, the manner by which such systems evolve towards their asymptotic superdiffusive behavior is explored using the 1d Lévy walk of order . The approach towards superdiffusion, as captured by the leading correction to the asymptotic behavior, is shown to remarkably undergo a transition as crosses the critical value . Above , this correction scales as , describing simple diffusion. However, below it is instead found to remain superdiffusive, scaling as . This transition is shown to be independent of the precise model details and is thus argued to be universal.
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