Authors: Carl P Dettmann
Publish Date: 2011/11/19
Volume: 146, Issue: 1, Pages: 181-204
Abstract
The Lorentz gas is a billiard model involving a point particle diffusing deterministically in a periodic array of convex scatterers In the two dimensional finite horizon case in which all trajectories involve collisions with the scatterers displacements scaled by the usual diffusive factor sqrtt are normally distributed as shown by Bunimovich and Sinai in 1981 In the infinite horizon case motion is superdiffusive however the normal distribution is recovered when scaling by sqrt tln t with an explicit formula for its variance Here we explore the infinite horizon case in arbitrary dimensions giving explicit formulas for the mean square displacement arguing that it differs from the variance of the limiting distribution making connections with the Riemann Hypothesis in the small scatterer limit and providing evidence for a critical dimension d=6 beyond which correlation decay exhibits fractional powers The results are conditional on a number of conjectures and are corroborated by numerical simulations in up to ten dimensions
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