M. Paczuski et al., AVALANCHE DYNAMICS IN EVOLUTION, GROWTH, AND DEPINNING MODELS, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, 53(1), 1996, pp. 414-443
The dynamics of complex systems in nature often occurs in terms of pun
ctuations, or avalanches, rather than following a smooth, gradual path
. A comprehensive theory of avalanche dynamics in models of growth, in
terface depinning, and evolution is presented. Specifically, we includ
e the Bak-Sneppen evolution model, the Sneppen interface depinning mod
el, the Zaitsev flux creep model, invasion percolation, and several ot
her depinning models into a unified treatment encompassing a large cla
ss of far from equilibrium processes. The formation of fractal structu
res, the appearance of 1/f noise, diffusion with anomalous Hurst expon
ents, Levy flights, and punctuated equilibria can all be related to th
e same underlying avalanche dynamics. This dynamics can be represented
as a fractal in d spatial plus one temporal dimension. The complex st
ate can be reached either by tuning a parameter, or it can be self-org
anized. We present two exact equations for the avalanche behavior in t
he latter case. (1) The slow approach to the critical attractor, i.e.,
the process of self-organization, is governed by a ''gap'' equation f
or the divergence of avalanche sizes. (2) The hierarchical structure o
f avalanches is described by an equation for the average number of sit
es covered by an avalanche. The exponent gamma governing the approach
to the critical state appears as a constant rather than as a critical
exponent. In addition, the conservation of activity in the stationary
state manifests itself through the superuniversal result eta = 0. The
exponent pi for the Levy flight jumps between subsequent active sites
can be related to other critical exponents through a study of ''backwa
rd avalanches.'' We develop a scaling theory that relates many of the
critical exponents in this broad category of extremal models, represen
ting different universality classes, to two basic exponents characteri
zing the fractal attractor. The exact equations and the derived set of
scaling relations are consistent with numerical simulations of the ab
ove mentioned models.