The transport times tau(P) and the mean free paths of magnetoexcitons
in a quantum well and of spatially direct and indirect magnetoexcitons
in coupled quantum wells in a random potential produced by thickness
fluctuations of the quantum wells or a random distribution of impurity
centers in quantum wells (P is the magnetic momentum of an exciton) a
re calculated. The function tau(P) is nonmonotonic, but as the distanc
e D between the quantum wells increases, the maximum tau(max)(P) gradu
ally vanishes in the presence of scattering by surface terraces. As th
e magnetic field (H) increases, tau(0) decreases as 1/root H for D muc
h less than l (l = root (h) over bar c/eH is the magnetic length) and
as 1/H-2 for D much greater than l. The behavior of the computed value
s of tau for large H agrees qualitatively with the experimental data.
The mean free path length of a magnetoexciton exhibits at P not equal
0 a maximum whose magnitude decreases as the parameter D/l increases,
(C) 1998 American Institute of Physics. [S1063-7826(98)01805-5].