A general framework is presented for the discussion of Brownian motion
in crystals with randomly distributed topological defects. In a two-d
imensional lattice with disclinations one finds a nonuniversal subdiff
usional behavior if screening in the disclination ensemble is taken in
to account. Without screening, a Sinai-type diffusion is expected. In
a three-dimensional random array of parallel screw dislocations, a Bro
wnian particle shows anisotropic normal diffusion. However, the proces
s no longer is Gaussian and displays long-time tails in the fourth-ord
er cumulants.