Abstract

We propose an approximate set of kinetic equations to describe the time evolution of spin correlation functions below T c in a system with long-range interactions. In the ordered region, these equations lead to weakly damped spin waves, in exact agreement with the previous work of Vaks, Lakkin and Pikin. When T c is approached, spin waves persist for q ⪡ κ_, where κ_is the inverse correlation length but, for q ⪢ κ_, these kinetic equations continuously transform into the non-Markoffian equation previously derived by one of the authors and De Leener above F c . Moreover, dynamical scaling is microscopically justified in our model. Beyond the assumption of a large number of interacting neighbours, we also need the phenomenological hypothesis that, close to T c , the equilibrium properties appearing in our kinetic equations can be described by their correct (nonclassical) critical indices.

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