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
using inverse fourier transfor-
mation (refer Sect. 1.2 ) , followed by back-projection technique.
(
x
,
y
)
by getting R
(
l
,θ)
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