The Boltzmann equation, Besov spaces, and optimal time decay rates in [formula omitted

Abstract

We prove that k-th order derivatives of perturbative classical solutions to the hard and soft potential Boltzmann equation (without the angular cut-off assumption) in the whole space, Rxn with n≥3, converge in large time to the global Maxwellian with the optimal decay rate of O(t−12(k+ϱ+n2−nr)) in the Lxr(Lv2)-norm for any 2≤r≤∞. These results hold for any ϱ∈(0,n/2] as long as initially ‖f0‖B˙2−ϱ,∞Lv2<∞. In the hard potential case, we prove faster decay results in the sense that if ‖Pf0‖B˙2−ϱ,∞Lv2<∞ and ‖{I−P}f0‖B˙2−ϱ+1,∞Lv2<∞ for ϱ∈(n/2,(n+2)/2] then the solution decays the global Maxwellian in Lv2(Lx2) with the optimal large time decay rate of O(t−12ϱ).