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4.4.1. Linear Elements
Consider a set of n = 2 m linear elements, half of which are general recep-
tors and the other half general effectors. A weak geometrical constraint,
which does not affect the generality of some of the following theorems but
facilitates description, is to assume spatial separation of receptors and effec-
tors. The locus of all general receptors, e 1 i , we shall call “transmitting layer”
L 1 , and the locus of all general effectors, e 2 j ,( i , j = 1,2,3,..., m ) the “col-
lecting layer” L 2 , regardless of the dimensionality of these loci, i.e., whether
these elements are arranged in a one-dimensional array, on a two-
dimensional surface, or in a specifiable volume.
We consider the fraction of activity in element e 1 i that is passed on to an
element e 2 i as its partial stimulus a ij ( i ). The action coefficients for the m 2
pairs define the numerical action matrix
(75)
A mij
=
.
m
With linear elements in the collector layer their responses are the algebraic
sum of their partial stimuli:
m
Â
() =
()
r
j
a
s
i
,
(76)
ij
i
or in a matrix notation
r
s
mmm
=
A
.
(77)
Since this result is in complete analogy to interaction nets (eq. (74))
where the response matrix R n establishes the stimulus-response relation-
ship, we have the following theorem:
Any stable interaction network composed of m elements can be repre-
sented by a functionally equivalent action network composed of 2 m ele-
ments (see fig. 23):
FIGURE 23. Equivalence of action network with interaction network.
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