Graphics Programs Reference
In-Depth Information
coherently. In this manner the information sequence
{
b () m
;
=
02 N
,
–
1
}
is
computed, where
b 2 N
(
–
1
)
is set to zero. At the same time one forms the
sequence
{
c () m
;
=
0 …2 N
,
–
2
}
which keeps track of the number of
returns that have the same
(
x n 1
+
x n 2
)
sum. More precisely, for
m 1
=
+
n 2
;
(
n 1 n 2
,
) 0 N
=
,
–
1
b () b () Ex n 1
=
+
(
,
x n 2
)
(12.55)
c () c ()1
=
+
(12.56)
It follows that
m
+
1
;
m
=
0 … N
,
–
2
{
c () m
;
=
0 …2 N
,
–
2
}
=
Nm
;
=
N
–
1
(12.57)
2 N
–
1
–
mm
=
N …2 N
,
–
2
which is a triangular shape sequence.
The processing of the sequence is performed as follows: (1) the
weighting takes the sequence into account; (2) the complex sequence
is extended to size , a power integer of two, by zero padding; (3)
the DFT of the extended sequence
{
b ()
}
{
c ()
}
{
b ()
}
N F
{
b ' ();
=
0 N F
,
–
1
}
is computed,
N F
–
1
j qm
N F
;
--------------
B ()
=
b ' () exp
–
=
0 … N F
,
–
1
(12.58)
m
=
0
and, (4) after compensation for antenna gain and range attenuation, scatterers
are detected as peaks in the amplitude spectrum
B ()
. Note that step (4) is
true only when
λ q
2 Nd
sin
β q
=
---------- ;
=
0 …2 N
,
–
1
(12.59)
where
sin
β q
denotes the direction-sine of the
q th
scatterer, and
N F
=
2 N
is
implied in Eq. (12.59).
The classical approach to multiple target detection is to use a phased array
antenna with phase shifting and tapering hardware. The array beamwidth is
proportional to , and the first sidelobe is at about -13 dB. On the other
hand, multiple target detection using DFTSQM provides a beamwidth propor-
tional to as indicated by (Eq. (12.59), which has the effect of dou-
bling the arrayÓs resolution. The first sidelobe is at about -27 dB due to the
triangular sequence . Additionally, no phase shifting hardware is
required for detection of targets within a single elementÓs field of view.
(
λ Nd
)
(
λ 2 Nd
)
{
c ()
}
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