  We consider interacting particle dynamics with Vicsek type interactions, and
their macroscopic PDE limit, in the non-mean-field regime; that is, we consider
the case in which each particle/agent in the system interacts only with a
prescribed subset of the particles in the system (for example, those within a
certain distance). In this non-mean-field regime the influence between agents
(i.e. the interaction term) can be normalised either by the total number of
agents in the system (\textit{global scaling}) or by the number of agents with
which the particle is effectively interacting (\textit{local scaling}). We
compare the behaviour of the globally scaled and the locally scaled systems in
many respects, considering for each scaling both the PDE and the corresponding
particle model. In particular we observe that both the locally and globally
scaled particle system exhibit pattern formation (i.e. formation of
travelling-wave-like solutions) within certain parameter regimes, and generally
display similar dynamics. The same is not true of the corresponding PDE models.
Indeed, while both PDE models have multiple stationary states, for the globally
scaled PDE such (space-homogeneous) equilibria are unstable for certain
parameter regimes, with the instability leading to travelling wave solutions,
while they are always stable for the locally scaled one, which never produces
travelling waves. This observation is based on a careful numerical study of the
model, supported by further analysis.
