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).