A method for investigating relaxation phenomena for charge-carrier hopping
between localized tail states is developed. It allows us to consider both c
harge and energy dispersive transport. The method is based on the idea of q
uasielasticity: the typical energy loss during a hop is much less than all
other characteristic energies. We investigate two models with different den
sity-of-state energy dependencies with our method. In general, we find that
the motion of a packet in energy space is affected by two competing tenden
cies. First, there is a packet broadening, i.e., dispersive energy transpor
t. Second, there is a narrowing of the packet if the density of states is d
epleting with decreasing energy. It is the interplay of these two tendencie
s that determines the overall evolution. If the density of states is consta
nt, only broadening exists. In this case a packet in energy space evolves i
nto a Gaussian one, moving with a constant drift velocity and mean-square d
eviation increasing linearly in time. If the density of states depletes exp
onentially with decreasing energy, the motion of the packet slows down trem
endously with time. For large times the mean-square deviation of the packet
becomes constant, so that the motion of the packet is "solitonlike."