“…and approximation by point vortices systems, [13,14,15,16]. The latter ones are defined, let us say first on T 2 , as systems of N point particles with positions x i ∈ D and intensities ξ i ∈ R, satisfying the system of ordinary differential equations ẋi,t = − j =i ξ j ∇ ⊥ G(x i,t , x j,t ),…”