“…Therefore, according to the previous considerations, the Vlasov-Poisson periodic problem consists in finding a couple (f, E), smooth enough, periodic with respect to x, with period L, which solves the equations (2), (7), (8), and (9). Introducing the electrostatic potential φ = φ(t, x) such that E(t, x) = −∂ x φ(t, x), and denoting by G = G(x, y) the fundamental solution of the Laplacian operator in one dimension…”