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Figure 7.1.
A set of interacting two-state nodes forms a small web. The two-headed arrows indicate the
interactions among the two-state nodes.
Let us imagine that each node of the given network is a dynamical unit described
by the master equation ( 7.9 ). To establish a dynamical connection among the nodes of
this network imagine that a given unit is influenced by all the other units to which it
is directly connected. In Figure 7.1 we illustrate this condition, where node 1 interacts
directly with nodes 4 and 5 and indirectly with nodes 2 and 3. As a consequence of
these interactions one possible choice for the coupling coefficients in ( 7.9 )istousethe
time-dependent transition probabilities per unit time given by [ 15 , 64 ]
g ij (
t
) =
g exp
(
K
[ π j (
t
) π i (
t
) ] ).
(7.11)
Note that in the Ising model mentioned earlier, a model used extensively in condensed-
matter physics, all the coupling coefficients are constants and we emphasize that this is
not the case being considered here. The weighting factors in the interaction coefficient
( 7.11 ) are given by the relative number of sites in the indicated state, that is,
M r
M ,
π r
=
(7.12)
where M r is the number of sites of that specific subset that are in the state r
2
and M denotes the total number of nodes connected to the site which is being con-
sidered. For instance M
=
1
,
2 in the case in which the site we are considering is site
1 of Figure 7.1 . The parameter K is the control parameter in the exponential ( 7.11 )
generating the coupling factor
=
exp K π j (
.
C ij =
t
) π i (
t
)
(7.13)
To illustrate what we mean, let us assume that the site we are considering, namely
site 1 in our example, is in the state r
1. Assume that both sites linked to it are in the
same state. In this situation the coupling factor is e 2 K . Thus, site 1 tends to remain in
the state r
=
1 for a more extended time than it would in the absence of any coupling.
If both linked sites are in the state r
=
2, the coupling factor is e 2 K , and site 1 makes a
=
transition from state r
=
1 to state r
=
2 earlier than it would in the absence of coupling.
When site 4 is in the state r
=
1( r
=
2) and site 5 is in the state r
=
2( r
=
1), site 1
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