Relaxation phenomena in disordered systems are often described by stre
tched exponentials; such behavior has traditionally been explained by
invoking statistical distributions. In hydrogenated amorphous silicon,
the relaxation has been associated with dispersive diffusion of hydro
gen, related to a distribution of energies for trap states and barrier
heights. Here we show that invoking such energy distributions is unne
cessary; a treatment of hydrogen motion which includes retrapping lead
s to a functional form of the decay curve which closely resembles a st
retched exponential, and provides an excellent fit to experimental dat
a. The implications of the new microscopic model are discussed.