We study self-diffusion within a simple hopping model for glassy materials.
(The model is Bouchaud's model of glasses (J.-P. Bouchaud, J. Phys. I Fran
ce 2, 1705 (1992)), as extended to describe rheological properties (P. Soll
ich, F. Lequeux, P. Hebraud, M.E. Cates, Phys. Rev. Lett. 78, 2020 (1997)).
) We investigate the breakdown, near the glass transition, of the (generali
zed) Stokes-Einstein relation between self-diffusion of a tracer particle a
nd the (frequency-dependent) viscosity of the system as a whole. This stern
s from the presence of a broad distribution of relaxation times of which di
fferent moments control diffusion and rheology. We also investigate the eff
ect of how (oscillatory sheer) on self-diffusion and show that this causes
a finite diffusivity in the temperature regime below the glass transition (
where this was previously zero). At higher temperatures the diffusivity is
enhanced by a power law frequency dependence that also characterises the rh
eological response. The relevance of these findings to soft glassy material
s (foams, emulsions etc.) as well as to conventional glass-forming liquids
is discussed.