Biomedical Engineering Reference
In-Depth Information
ʣ y is given by
However,
N
ʣ y = ʲ 1 I
L j ʥ j L j ,
+
(4.74)
j
=
1
where the M
×
3 lead fieldmatrix at the j th voxel, L
(
r j )
, is denoted L j for simplicity.
In agreement with Eq. ( 4.49 ), since log
| ʣ y |
is a concave function, we can find
3
×
3 auxiliary parameter matrices, Z j ,( j
=
1
,...,
N ) that satisfy
N
tr Z j ʥ j
Z o
log
| ʣ y | ,
(4.75)
j
=
1
where Z o is a scalar term that depends on Z j . Regarding the second term in the
right-hand side of Eq. ( 4.73 ), we have the relationship
x k ʥ 1 x k
y k ʣ 1
2
y k =
min
x k
ʲ
y k
Fx k
+
y
ʲ
.
N
t k ) ʥ 1
2
s j (
=
min
x k
y k
Fx k
+
s j (
t k )
(4.76)
j
j
=
1
Let us use Z to collectively express Z 1 ,...,
Z N , and use s to collectively express
s j (
t k )
, where j
=
1
,...,
N and k
=
1
,...,
K . The alternative cost function,
F( ʥ ,
s
,
Z
)
, is obtained as
K
N
1
K
F( ʥ ,
ʲ
2
t k ) ʥ 1
s j (
s
,
Z
) =
y k
Fx k
+
s j (
t k )
j
k
=
1
j
=
1
tr Z j ʥ j
N
+
Z o .
(4.77)
j =
1
This F( ʥ ,
forms an upper bound of the true cost function in Eq. ( 4.73 ). Accord-
ingly, when we minimize F( ʥ ,
s
,
Z
)
s
,
Z
)
with respect to
ʥ
, s , and Z , we can minimize
the true cost function
F( ʥ )
.
4.8.1 Update Equation for Z j
Using the same arguments in Sect. 4.6.2 , the update equation for Z j is derived as
ʥ j
Z j
=
log
| ʣ y | .
(4.78)
 
 
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