Fractional diffusion as the limit of a short range potential Rayleigh gas

The fractional diffusion equation is rigorously derived as a scaling limit from a deterministic Rayleigh gas, where particles interact via short range potentials with support of size $\epsilon$ and the background is distributed in space ${\mathbb{R}}^3$ according to a Poisson process with intensity $N$ and in velocity according to some fat-tailed distribution. As an intermediate step a linear Boltzmann equation is obtained in the Boltzmann-Grad limit as $\epsilon$ tends to zero and $N$ tends to infinity with $N{\epsilon }^2=c$. The convergence of the empiric particle dynamics to the Boltzmann-type dynamics is shown using semigroup methods to describe probability measures on collision trees associated to physical trajectories in the case of a Rayleigh gas. The fractional diffusion equation is a hydrodynamic limit for times $t\in [0,T]$, where $T$ and inverse mean free path $c$ can both be chosen as some negative rational power ${\epsilon }^{-k}$.