Abstract

We prove a superdiffusive central limit theorem for the displacement of a test particle in the periodic Lorentz gas in the limit of large times tt and low scatterer densities (Boltzmann-Grad limit). The normalization factor is tlog⁡t\sqrt{t\log t}, where tt is measured in units of the mean collision time. This result holds in any dimension and for a general class of finite-range scattering potentials. We also establish the corresponding invariance principle, i.e., the weak convergence of the particle dynamics to Brownian motion.

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