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It is equivalent to write (16)-(17) with the form of
d
=(
d
1
,d
2
)and
b
=(
b
1
,b
2
).
d
1
+
d
2
d
x
(
ˈ
n
+1
,d
n
+1
1
,d
n
+1
2
)=arg min
ˈ,d
1
,d
2
ʩ
+
μ
2
d
x
+
ʻ
2
ˈ
)
2
b
1
)
2
d
x
(1
−
|∇
u
|
(
d
1
−
∂
x
ˈ
−
(18)
ʩ
ʩ
b
2
)
2
d
x
,
+
ʻ
2
(
d
2
−
∂
y
ˈ
−
ʩ
and
=
b
1
+
∂
x
ˈ
n
+1
,
n
+1
2
=
b
2
+
∂
y
ˈ
n
+1
.
b
n
+1
1
d
n
+1
1
d
n
+1
2
−
−
The Euler-Lagrange equation of (18) for
ˈ
with fixed
d
1
and
d
2
is
2
(
ˈ
b
1
)
b
2
)=0
,
−
ʻʔˈ
+2
μ
|∇
u
|
−
1)
−
ʻ∂
x
(
d
1
−
−
ʻ∂
y
(
d
2
−
with the Neumann boundary conditions
∂ˈ
∂
n
=0
.
Applying the same technique
in Subsection 2.1, we need to solve the equations about
ˈ
:
i,j
=
ˈ
k
+
ˉ
2
F
i,j
+
ʻ
(
ˈ
i
+1
,j
+
ˈ
k
+1
i,j−
1
+
ˈ
i,j
+1
)
i−
1
,j
+
ˈ
k
+1
ˈ
k
+1
,
(19)
u
)
k
+1
i,j
1+
ˉ
2
(2
μ
|
∇
|
2
+4
ʻ
)
(
where
ˉ
2
>
0 is the relaxation factor and
2
+
ʻ∂
x
(
d
1
−
b
1
)+
ʻ∂
y
(
d
2
−
b
2
)
.
F
:= 2
μ
|∇
u
|
For fixed
ˈ
, the optimality condition of (18) with respect to
d
1
and
d
2
gives
d
1
=max
h
ʻ
,
0
h
1
h
,
2
=max
h
ʻ
,
0
h
2
1
1
−
−
h
,
(20)
where
h
1
=
∂
x
ˈ
+
b
1
,
2
=
∂
y
ˈ
+
b
2
, h
=
h
1
+
h
2
.
Now, we summarize the split Bregman (SB) algorithm as follows.
Split Bregman Algorithm
1. Initialization: set
d
1
=
d
2
=
b
1
=
b
2
=0
,
and input
ˈ
0
,u
0
,μ,ʽ,ˉ
1
,ˉ
2
,ʻ.
2. For
n
=0
,
1
,
,
(i) Update
u
n
+1
using the iteration scheme (13) with initial value for iter-
ation:
u
n
and
ˈ
n
(in place of
ˈ
);
(ii) Update
g
n
by
···
n
max
0
,
1
;
1
g
n
=
|
u
−
I
|
−
ʾ
|
(
u
−
I
)
n
|
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