Lo. Chua et al., AUTONOMOUS CELLULAR NEURAL NETWORKS - A UNIFIED PARADIGM FOR PATTERN-FORMATION AND ACTIVE WAVE-PROPAGATION, IEEE transactions on circuits and systems. 1, Fundamental theory andapplications, 42(10), 1995, pp. 559-577
This tutorial paper proposes a subclass of cellular neural networks (C
NN) having no inputs (i.e., autonomous) as a universal active substrat
e or medium for modeling and generating many pattern formation and non
linear wave phenomena from numerous disciplines, including biology, ch
emistry, ecology, engineering, physics, etc. Each CNN is defined mathe
matically by its cell dynamics (e.g., state equations) and synaptic la
w, which specifies each cell's interaction with its neighbors. We focu
s in this paper on reaction-diffusion CNNs having a linear synaptic la
w that approximates a spatial Laplacian operator. Such a synaptic law
can be realized by one or more layers of linear resistor couplings. An
autonomous CNN made of third-order universal cells and coupled to eac
h other by only one layer of linear resistors provides a unified activ
e medium for generating trigger (autowave) waves, target (concentric)
waves, spiral leaves, and scroll waves. When a second layer of linear
resistors is added to couple a second capacitor voltage in each cell t
o its neighboring cells, the resulting CNN can be used to generate var
ious turing patterns. Although the equations describing these autonomo
us CNNs represent an excellent approximation to the nonlinear partial
differential equations describing reaction-diffusion systems if the nu
mber of cells is sufficiently large, they can exhibit new phenomena (e
.g., propagation failure) that can not be obtained from their limiting
partial differential equations. This demonstrates that the autonomous
CNN is in some sense more general than its associated nonlinear parti
al differential equations. To demonstrate how an autonomous CNN can se
rve as a unifying paradigm for pattern formation and active wave propa
gation, several well-known examples chosen from different disciplines
are mapped into a generic reaction-diffusion CNN made of third-order c
ells. Finally, several examples that can not be modeled by reaction-di
ffusion equations are mapped into other classes of autonomous CNNs in
order to illustrate the universality of the CNN paradigm.