Image Processing Reference
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B 0
Precessional
motion
µ
Spin motion
FIGURE 1.2
Precession of nuclear magnetic moment about the magnetic field
B
.
0
, the orientation of the spin
angular momentum vector, and hence the magnetic moment, of the nucleus with
respect to the direction of
According to the
quantum mechanical model
cannot be arbitrary and it is subjected to certain
restrictions. In fact, the nuclear magnetic moment can only have 2I + 1 orientations
in a magnetic field, corresponding to 2I
B
0
+
1 allowed energy levels, so that the
proton (
H) nucleus can either align with or against the applied field. These two
orientations are similar to the two directions in which a bar magnet may orient in
a magnetic field and are consequently called the parallel (spin-up) and the anti-
parallel (spin-down) orientations. These orientations correspond to low and high
1
energy states respectively, as schematically shown in Figure 1.3 .
The difference in energy,
E
, between the two states is proportional to the
strength of the magnetic field
B
, and it is given by
0
E
=
γ
B
(1.6)
0
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