Smoothness of the Solution of the Spatially Homogeneous Boltzmann Equation Without Cutoff.

For regularized hard potentials cross sections, the solution of the spatially homogeneous Boltzmann equation without angular cutoff lies in Schwartz's space T(RN) for all (strictly positive) time. The proof is presented in full detail for the two-dimensional case, and for a moderate singularity of the cross section. Then we present those parts of the proof for the general case, where the dimension, or the strength of the singularity play an essential role. [ABSTRACT FROM AUTHOR]