Digital Signal Processing Reference
In-Depth Information
Appendix A
Solving Bloch Equation with ADvsinc
ð
Dvt
Þ
Envelope
condition Dv\\
B
0
c
2p
.
dM
xy
ð
t
Þ
dt
¼
jcADvsinc
ð
Dvt
Þ
M
0
cos
ð
a
Þ
e
j
ð
cB
0
t
þ
h
Þ
ð
A
:
1
Þ
dM
z
ð
t
Þ
dt
ð
A
:
2
Þ
¼
cADvsinc
ð
Dvt
Þ
M
0
sin
ð
a
Þ
E
0
sin
ð
h
/
Þ
Since sinc
ð
Dvt
Þ
is almost one for all t with Dv\\
B
0
c
2p
, we treat sinc
ð
Dvt
Þ
as the
constant in both the equations and solution is obtained as follows
M
xy
ð
t
Þ¼
2M
0
sin
ð
a
Þ
e
j
ð
cB
0
t
þ
/
Þ
ð
A
:
3
Þ
M
z
ð
t
Þ¼
cM
0
sin
ð
a
Þ
ADvsinc
ð
Dvt
Þ
sin
ð
h
/
Þ
t
þ
2M
0
cos
ð
a
Þ
ð
A
:
4
Þ
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