Digital Signal Processing Reference
In-Depth Information
Fig. 3.6
a
Illustrating the order in which the K-space is scanned;
b
sample polar scanned K-space
9. Apply inverse fourier transformation in polar form to obtain
f
(
x
,
y
)
(refer
Sect.
3.3.1
).
10. For checking the validity of reconstruction from polar data,
k
is chosen as zero
matrix (No dephasing) for illustration. This helps to obtain proton-density image
(n-matrix) as the reconstructed image.
3.3.1 Reconstructing f
(
x
,
y
)
from G
(
r
,θ)
There are two major techniques to obtain
f
namely back-
projection technique and the interpolation technique as described below. The
interpolation technique is used for illustration purpose.
(
x
,
y
)
from
G
(
r
,θ)
3.3.1.1 Back-Projection Technique
The generalized formula to reconstruct
f
(
x
,
y
)
from
G
(
r
,θ)
is as shown below.
π
∞
exp
j
2
π(
xcos
θ
+
ysin
θ)
r
f
(
x
,
y
)
=
G
(
r
,θ)
|
J
|
drd
θ
(3.2)
−
π
0
1. It it noted
G
(
r
,θ)
is the fourier transformation of the radon transformation
R
(
l
,θ)
for the specific constant
θ
.
2. It is possible to get back
f
(
x
,
y
)
by getting
R
(
l
,θ)
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