From a microscopic point of view the fundamental theory about this problem is given in (1). In that theory, however, the detailed balance relation, postulated in phenomenological work (2, 3), is violated (4). The way, proposed in (4), to overcome this discrepancy i s not satisfactory.In the followir;g, the dynamic transverse susceptibility i s calculated from a microscopic starting point. The results satisfy the law of detailed balance. For the bottleneck (3) relaxation rate a temperature independent term being of first order in the exchange parameter, results from this law.