Biomedical Engineering Reference
In-Depth Information
(
)
(
×
)
where A
p
is a
2
2
coefficient matrix. We can derive Eq. ( 8.7 ), which is explicitly
written as
x
H xx H xy
H yx H yy
e x (
(
f
)
f
)
=
.
(8.46)
y
(
f
)
e y (
f
)
In the expressions above, the explicit notation of the frequency f is omitted from
the components of H
(
f
)
. Denoting the residual covariance matrix such that
Σ x
2
)
|
e x (
f
) |
e x (
f
)
e y (
f
ʳ
=
,
(8.47)
) |
ʳ
2
e y (
f
)
e x (
f
e y (
f
) |
Σ y
where the superscript
indicates the complex conjugation. Equation ( 8.8 ) is explicitly
written as
H Σ x
H H
2
)
|
x
(
f
) |
x
(
f
)
y
(
f
ʳ
=
.
(8.48)
) |
2
ʳ
y
(
f
)
x
(
f
y
(
f
) |
Σ y
8.4.2 Total Interdependence and Coherence
We first define the total interdependence between x and y , which corresponds to
I { x , y } in Eq. ( 8.40 ). Using the arguments in Sect. 8.3.3 , the total interdependence
between x and y in the spectral domain is defined as
2
|
x
(
f
) |
0
2
0
|
y
(
f
) |
f
} =
log
{
x
,
y
|
S
(
f
) |
2
2
|
x
(
f
) |
|
y
(
f
) |
=
log
2 .
(8.49)
2
2
) |
|
x
(
f
) |
|
y
(
f
) |
−|
x
(
f
)
y
(
f
Comparing the equation above to Eq. ( 7.40 ) in Chap. 7 , it can immediately be seen
that under the Gaussianity assumption, the spectral domain total interdependence is
equal to the mutual information discussed in Sect. 7.5.2 . Therefore, using the same
arguments, the total interdependence f
is related to the magnitude coherence
{
x
,
y
}
| ˆ(
f
) |
through
2
f
} (
f
) =−
log
(
1
−| ˆ(
f
) |
),
(8.50)
{
x
,
y
where
) |
2
|
x
(
f
)
y
(
f
2
| ˆ(
f
) |
=
.
(8.51)
2
2
|
x
(
f
) |
|
y
(
f
) |
 
 
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