Digital Signal Processing Reference
In-Depth Information
3.1.1 Proton-Density MRI Imaging
Let the image slice be represented as the matrix with the values filled up with proton-
density is as follows.
33979586994
559109551 7 910
69612992 6 9 6
56227822292
981109587101 5
61247378 1 3 9
99765479 034
53298946 5107
4138295109 4 6
59644217 8 9 7
48578314984
=
n
These are the magnitude of the resultant magnetic moment at t
0 (refer Fig. 3.4 ).
The following steps are followed to obtain the K-space corresponding to the proton-
density image. The identical transverse components are assumed to be available at
every pixel of the image slice, i.e. they are in-phase and are rotating in the Larmor
frequency.
=
1. Apply G y gradient for the duration of 0.0000000009.
2. Apply
G x gradient for the duration of 0.0000000009.
3. Apply G x gradient for the duration of 0.0000000018. During this phase, after the
time duration of 0.0000000009, there is the cancellation of phase introduced due
to G x . This is known as Gradient echo. This helps to synchronize the hardware
to sample at the particular instant during real time to choose the proper position
in the K-space.
4. Sample the real and imaginary component of the signal s
(
t
)
to obtain the sample
.
5. Proper scaling factor is used so that the final basis (to perform IFFT2) look like
the standard form e j 2 π xG x
of the K-space at
(
G x ,
G y )
e j 2 π yG y
11 . This is the process of discretization.
6. The above steps are repeated for the complete scan in the K-space. For every
time, we have to wait for the longitudinal component to reach maximum before
applying 90 RF pulse. (This is illustrated by repeating the steps 1-5 by varying
the values of G x and G y ranging from
11
5 to 5 with the interval of 1.)
The resultant KSPACE is obtained as follows.
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