In order to perform quantum Hamiltonian dynamics minimizing localization ef
fects, we introduce a quasi-one-dimensional tight-binding model whose mean
free path is smaller than the size of the sample. This size, in turn, is sm
aller than the localization length. We study the return probability to the
starting layer using direct diagonalization of the Hamiltonian. We create a
one-dimensional excitation and observe sub-diffusive behavior for times la
rger than the Debye time but shorter than the Heisenberg time. The exponent
corresponds to the fractal dimension d* similar to 0.72 which is compared
to that calculated from the eigenstates by means of the inverse participati
on number. (C) 2000 Elsevier Science B.V. All rights reserved.