Abstract
The Vlasov–Poisson system describes interacting systems of collisionless particles. For solutions with small initial data in three dimensions it is known that the spatial density of particles decays as t −3 at late times. In this paper this statement is refined to show that each derivative of the density which is taken leads to an extra power of decay, so that in N dimensions for $${N \geqq 3}$$ the derivative of the density of order k decays as t −N-k . An asymptotic formula for the solution at late times is also obtained.
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