We study the propagation of electrons (or excitations) through a one-dimens
ional tight-binding chain in the simultaneous presence of nonlinearity and
diagonal disorder. The evolution of the system is given by a disordered ver
sion of the discrete nonlinear Schrodinger equation. For an initially local
ized excitation we examine its mean square displacement [n(2)(t)] for relat
ively long times Vt similar to 10(4), for different degrees of nonlinearity
. We found that the presence of nonlinearity produces a subdiffusive propag
ation [n(2)(t)]similar to t(alpha), with alpha similar to 0.27 and dependin
g weakly on nonlinearity strength. This nonlinearity effect seems to persis
t for a long time before the system converges to the usual Anderson model.
We also compute the transmission of plane waves through the system. We foun
d an average transmissivity that decays exponentially with system size [T]s
imilar to exp(-beta L), where beta increases with nonlinearity. We conclude
that the presence of nonlinearity favors (inhibits) the propagation of loc
alized (extended) excitations. [S0163-1829(98)06340-1].