  We consider a two-dimensional Lorentz gas with infinite horizon. This
paradigmatic model consists of pointlike particles undergoing elastic
collisions with fixed scatterers arranged on a periodic lattice. It was
rigorously shown that when $t\to\infty$, the distribution of particles is
Gaussian. However, the convergence to this limit is ultraslow, hence it is
practically unattainable. Here we obtain an analytical solution for the Lorentz
gas' kinetics on physically relevant timescales, and find that the density in
its far tails decays as a universal power law of exponent $-3$. We also show
that the arrangement of scatterers is imprinted in the shape of the
distribution.
