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Fig. 15.1: ( a ) Unidirectionally coupled oscillators with
05. ( b ) Mutual in-
formation MI vs. k (the first minimum of the mutual information between the X
variables of the oscillators is denoted by a downward arrow at k
ε 21 =
0
.
=
16). ( c )ln C vs.
=
=
ln r with k
1, where C and r denote average joint probability and radius,
respectively ( dotted line for direction of flow 1
16, l
2; solid line for direction of flow
2
1). ( d ) Autocorrelation function (AF) vs. k (the delay at which the AF decreases
to 1
/
e of its maximum value is denoted by a downward arrow at k
=
14).
of the driving system is sufficient to produce a considerable change in the dynamics
of the driven system within one time step (and hence only immediate interactions
between X and Y are assumed to be detected in the analysis herein). When larger
values for l were employed (i.e., a delayed influence of Y on X ), detection of infor-
mation flow from Y to X was also possible. These results are not presented in this
chapter.
15.2.2.3 Selection of Radius r
The multi-dimensional transitional probabilities involved in the definition of transfer
entropy (Equation (15.3)) are calculated by joint probabilities using the conditional
probability formula P
(
A
|
B
)=
P
(
A
,
B
) /
P
(
B
)
. One can then reformulate the transfer
entropy as
TE
(
Y
X
)=
log 2 P ( x n + 1 , x ( k )
y ( l )
n
x ( k )
n
(15.4)
x ( k )
y ( l )
,
)
P
(
N
n
1 P
(
x n + 1 ,
,
)
n
.
n
n
=
P ( x n + 1 , x ( k )
) P ( x ( k )
n
, y ( l )
n
)
n
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