In solid He-3 the internuclear exchange interaction may be interpreted
as a molecular field, as in the Weiss theory of magnetism. In an appl
ied magnetic field the magnetic moment precesses about the total magne
tic field, to which the molecular field contributes. As Leggett showed
for liquid helium in the Fermi liquid region, this leads to a modific
ation of the time evolution of the magnetisation; it is no longer pure
ly diffusive. In solid He-3 at low polarisation there is conventional
spin diffusion; at high polarisations the evolution is in the form of
spin waves. We show that the intermediate behaviour may be expressed i
n terms of a complex diffusion coefficient of constant magnitude, whos
e phase angle depends on the polarisation.