Andrea Gabrielli — Università di Roma "La Sapienza" # Finite\(-N\) corrections to Vlasov dynamics and the range of pair interactions # We explore [1] the conditions on a pair interaction for the validity of the Vlasov equation to describe the dynamics of an interacting \(N\) particle system in the large \(N\) limit. Using a coarse-graining in phase space of the exact Klimontovich equation for such a system, we evaluate the scalings with \(N\) of the terms describing the corrections to the Vlasov equation for the coarse-grained one particle phase space density. Considering an interaction with radial pair force \(F(r)\sim1/ra\), regulated to a bounded behavior below a "softening" scale \(l\), we find that there is an essential qualitative difference between the cases \( a < d \) (i.e. the spatial dimension) and \(a > d\) , i.e., depending on the the integrability at large distances of \(F(r)\). For \( a < d \) the corrections to the Vlasov dynamics for a given coarse-grained scale are essentially insensitive to the softening parameter \(l\), while for \(a>d\) the corrections are directly regulated by \(l\), i.e. by the small scale properties of the interaction, in agreement with the Chandrasekhar approach [2]. This gives a simple physical criterion for a basic distinction between long-range (\( a < d \)) and short range (\(a>d\)) interactions, different from the thermodynamic one (\( a < d-1 \) or \( a > d-1 \)). This alternative classification, based purely on dynamical arguments, is relevant notably to understanding the conditions for the existence of so-called quasi-stationary states in long-range interacting systems.

[1] A. Gabrielli et al., Phys. Rev. E, 90, 062910 (2014).
[2] A. Gabrielli et al., Phys. Rev. Lett., 115, 210602 (2010).