Biomedical Engineering Reference
In-Depth Information
and using this column vector, coherence is expressed as 3
h j
ʣ
h k
S j , k
S j , j S k , k =
H
j
ˆ j , k (
f
) =
= ʳ
(
f
) ʣʳ k (
f
).
(8.69)
h j
h k
[
ʣ
h j ][
ʣ
h k ]
This directed coherence
ʳ j , k is known to represent the directional influence from
the k th to the j th channels. It contains the residual covariance matrix
whose off-
diagonal terms may represent the instantaneous interaction between two channels,
according to the arguments in Sect. 8.3.3 . Setting
ʣ
ʣ
equal to I ,wehave
H j , k (
f
)
ʳ j , k =
,
(8.70)
h j
|
h j |
which is exactly equal to the normalized DTF in Eq. ( 8.66 ). Namely, the DTF is a
measure for directional influences obtained by removing instantaneous components
from the directed coherence. Under the assumption that
ʣ =
I , coherence
ˆ j , k (
f
)
can be decomposed of the sum of the product of DTFs, such that
q
m
q
H k , m (
1 H j , m (
f
)
f
)
=
1 μ m j μ m k .
ˆ j , k (
f
) =
=
(8.71)
h j
h k
[
h j ][
h k ]
m
=
8.5.3 Partial Directed Coherence (PDC)
In Sect. 8.5.2 , DTF is expressed using a factorization of coherence. We apply similar
factorization to partial coherence to obtain the partial directed coherence (PDC)
[ 6 , 12 ]. The starting point is Eq. ( 8.14 ), which is re-written as,
ʣ 1
a j
¯
a k
¯
ʺ j , k (
f
) =
.
(8.72)
a j
ʣ 1
a k
ʣ 1
[ ¯
¯
a j ][ ¯
a k ]
¯
¯ A
=[ A 1 , j ,..., A q , j ]
Here, recall that
a j is the j th column of the matrix
¯
(
f
)
and
¯
a j
.
We define
A j , k (
f
)
ˀ j , k (
f
) =
a k ,
(8.73)
a k
ʣ 1
¯
¯
3
Note that since h j is the j th column vector of H H , h j is equal to h j
H j , 1 ,...,
H j , q ]
T .
=[
 
 
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