Mo. Vlad et al., GENERALIZED HUBER KINETICS FOR NONLINEAR RATE-PROCESSES IN DISORDERED-SYSTEMS - NONLINEAR ANALOGS OF STRETCHED EXPONENTIAL, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, 57(6), 1998, pp. 6497-6505
This paper deals with one-variable nonlinear rate processes occurring
in disordered systems. A general stochastic approach is introduced for
these processes based on the following assumptions. The total rate co
efficient is made up of the additive contributions of a large number o
f individual reaction channels. These contributions are random functio
ns of time and their stochastic properties are characterized by a func
tional random point process. Exact analytical expressions for the time
dependence of the average concentration are derived by using a charac
teristic functional technique. These expressions are valid for systems
with both dynamic and static disorder and are nonlinear analogs of th
e general kinetic law derived by Huber [Phys. Rev. B 31, 6070 (1985);
Phys. Rev. E 53, 6544 (1996)] for Linear rate processes in systems wit
h static disorder. Fbr independent rate processes with static disorder
and a self-similar distribution of reaction channels we derive a nonl
inear analog of the stretched exponential. A closed analytic expressio
n of the nonlinear stretched exponential is given in terms of Fox's H
functions. As expected, when the reaction order of the process is one,
the nonlinear kinetic law reduces to a stretched exponential with a s
caling exponent characterizing the self-similar distribution of the in
dividual reaction channels. For nonlinear processes the tail of the av
eraged kinetic curve is self-similar and obeys a scaling law with a ne
gative power law. Surprisingly, the scaling exponent of the tail depen
ds only on the reaction order of the process and is independent of the
scaling exponent that characterizes the self-similar distribution of
the individual channels. We examine the possibilities of experimental
evaluation of the statistical distribution of the total rate coefficie
nt: The moments of different orders of the rate coefficient can be eva
luated from the time derivatives of the survival function.