Scaling of the dynamics of a homogeneous one-dimensional anisotropic classical Heisenberg model with long-range interactions

The dynamics of quasi-stationary states of long-range interacting systems with $N$ particles can be described by kinetic equations such as the Balescu-Lenard and Landau equations. In the case of one-dimensional homogeneous systems, two-body contributions vanish as two-body collisions in one dimension only exchange momentum and thus cannot change the one-particle distribution. Using a Kac factor in the interparticle potential implies a scaling of the dynamics proportional to $N^{\delta }$ with $\delta =1$ except for one-dimensional homogeneous systems. For the latter different values for $\delta$ were reported for a few models. Recently it was show by Rocha Filho and collaborators [Phys.
Rev.\ E {\bf 90}, 032133 (2014)] for the Hamiltonian mean-field model that $\delta =2$ provided that $N$ is sufficiently large, while small $N$ effects lead to $\delta \approx 1.7$. More recently Gupta and Mukamel [J.\ Stat.\ Mech.
P03015 (2011)] introduced a classical spin model with an anisotropic interaction with a scaling in the dynamics proportional to $N^{1.7}$ for a homogeneous state. We show here that this model reduces to a one-dimensional Hamiltonian system and that the scaling of the dynamics approaches $N^2$ with increasing $N$. We also explain from theoretical consideration why usual kinetic theory fails for small $N$ values, which ultimately is the origin of non-integer exponents in the scaling.