Global Positioning System Reference
In-Depth Information
M
−
1
⎧
∑
∑
⎫
2
dM
d
=
i
⎪
⎪
i
k
=
0
⎪
⎪
S
d
R
=
⎨
(30)
()
i
M
⎬
∈
:
−
1
>
0
L
i
⎪
i
=
0
⎪
dd
=
,
k
=
, ,
,
M
−
1
⎪
⎪
⎩
⎭
k
Mk
−−
1
2
With an appropriate weight coefficient α, all the undesired positive side peaks of
2
R
can
be canceled by subtraction. From (18), the coefficient
α
must satisfies
M
−
k
(
)
α
r
≥
R TM
/
=
(31)
k
B
c
M
for
k
=
1, 2,
,
M
−
1
, or
M
−
k
α
≥
max
k
.
(32)
M r
≠
0
k
5.4 Step 4 - Local waveform optimization
So far the effect of thermal noise has not been considered. In fact, the coefficient α amplifies
noise components in
B/
R
. Under a given pre-correlation SNR, the larger α is, the lower
SNR in the SCF is. Therefore, from the viewpoint of sensitivity, it is desired that α be as
small as possible. So that with a given
d
the optimum α is
M
−
k
α
=
max
k
(33)
()
Mr
d
≠
0
k
L
and in UVS, the optimum
d
is the one minimizing α, that is
M
−
k
d
=
arg min
α
=
arg min max
(34)
opt
M r
d
∈
S
d
∈
S
k
≠
0
L
L
k
It can be proved that the explicit expression of (34) is
[
]
T
d
=
dd
,
,
d
−
(35)
opt
0
1
M
1
where
⎨
dd
=
=
M
−
1
0
M
−
1
23
1
M
−
(36)
i
−
1
()
(
)
−
dd
=
=
,
i
=
, ,
,
M
−
1
⎩
i
Mi
−+
1
2
23
M
−
and
α =−.
2
M
3
min
Figure 11 (a)-(c) depict the optimum local SCS waveforms for BOC(
n
,
n
), BOC(2
n
,
n
), and
BOC(3
n
,
n
) signals respectively. For BOC(
n
,
n
) signals,
( )
T
α = . It
can be found that the SC method proposed in (Julien, et al., 2007) is equivalent to this case.
The local symbol is simply a rectangular pulse. For BOC(2
n
,
n
),
M
=
.
So
2
d
=
1,1
and
1
min
opt
(
)
T
d
=
9
1,,,1
11
and
opt
5
3
3
(
)
T
α = . For BOC(3
n
,
n
),
5
d
=
1
5,1,
− −
1,
1,1, 5
and
α = . It can be seen that the
9
min
opt
min
3
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