Rate processes with dynamical disorder are investigated within a simple
framework provided by unidirectional electron transfer (ET) with fluctuating
transfer rate. The rate fluctuations are assumed to be described by a
non-Markovian stochastic jump process which reflects conformational dynamics of
an electron transferring donor-acceptor molecular complex. A tractable
analytical expression is obtained for the relaxation of the donor population
(in the Laplace-transformed time domain) averaged over the stationary
conformational fluctuations. The corresponding mean transfer time is also
obtained in an analytical form. The case of two-state fluctuations is studied
in detail for a model incorporating substate diffusion within one of the
conformations. It is shown that an increase of the conformational diffusion
time results in a gradual transition from the regime of fast modulation
characterized by the averaged ET rate to the regime of quasi-static disorder.
This transition occurs at the conformational mean residence time intervals
fixed much less than the inverse of the corresponding ET rates. An explanation
of this paradoxical effect is provided. Moreover, its presence is also
manifested for the simplest, exactly solvable non-Markovian model with a
biexponential distribution of the residence times in one of the conformations.
The nontrivial conditions for this phenomenon to occur are found