Systems with long-range interactions often relax towards statistical equilibrium over timescales that diverge with N , the number of particles. A recent work (Gupta and Mukamel 2011 J. Stat. Mech. P03015) analyzed a model system comprising N globally coupled classical Heisenberg spins and evolving under classical spin dynamics. It was numerically shown to relax to equilibrium over a time that scales superlinearly with N . Here, we present a detailed study of the Lenard–Balescu operator that accounts at leading order for the finite- N effects driving this relaxation. We demonstrate that corrections at this order are identically zero, so that relaxation occurs over a time longer than of order N , in agreement with the reported numerical results.
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