Mo. Vlad et al., SELF-SIMILAR POTENTIALS IN RANDOM-MEDIA, FRACTAL EVOLUTIONARY LANDSCAPES AND KIMURAS NEUTRAL THEORY OF MOLECULAR EVOLUTION, Physica. A, 229(3-4), 1996, pp. 343-364
A general method for constructing self-similar scalar fractal random f
ields is suggested based on the assumption that the fields are generat
ed by a broad distribution of punctual sources. The method is illustra
ted by a problem of population biology, the evolution on a random fitn
ess landscape. A random fitness landscape is constructed based on the
following hypotheses. The landscape is defined by the dependence of a
fitness variable phi on the state vector x of the individuals: phi = p
hi(x); the corresponding hypersurface has a large number of local maxi
ma characterized by a local probability law with variable parameters.
These maxima are uniformly randomly distributed throughout the state s
pace of the individuals. From generation to generation the heights and
the shapes of these local maxima can change; this change is described
in terms of two probabilities p and alpha that an individual modifica
tion occurs and that the process of variation as a whole stops, respec
tively. A general method for computing the stochastic properties of th
e evolutionary landscape is suggested based on the use of characterist
ic functionals. An explicit computation of the Fourier spectrum of the
cumulants of the evolutionary landscape is performed in a limit of th
e thermodynamic type for which the number of maxima and the volume of
the state space of the individuals tend to infinity but the density of
maxima remains constant. It is shown that, although a typical realiza
tion of the evolutionary landscape is very rough, its average properti
es expressed by the Fourier spectrum of its cumulants are smooth and c
haracterized by scaling laws of the power law type. The average landsc
ape which is made up of the frozen contributions of the changes corres
ponding to different generations is flat, a result which is consistent
with the Kimura's theory of molecular evolution. Some general implica
tions of the suggested approach for the statistical physics of systems
with random ultrametric topology are also investigated.