  Combining the results of [14] and [10], the trend to equilibrium in large
time is studied for a large particle system associated to a
Vlasov-Fokker-Planck equation. Under some conditions (that allow non-convex
confining potentials) the convergence rate is proven to be independent from the
number of particles. From this are derived uniform in time propagation of chaos
estimates and an exponentially fast convergence for the nonlinear equation
itself.
