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An Experimental Approach to CDMA and Interference Mitigation phần 5 doc
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3. Design of an All Digital CDMA Receiver 97
BB
BB
0.61 0.1525
4
c
d c
B R
f R E , (3.38)
which does not depend on the chip rate. Figure 3-12 shows the generic
frequency response G f ( ), as compared with the various (wanted and
unwanted) spectral components of the received signal.
… z
-1
Stage 2
Decimation
U
Stage ( UM-1)
fs fd
z
-1
z
-1 z
-1
Stage 1
FIR 1
FIR 2
FIR 3
…
FIR N
fs
S(z) H(z)
Figure 3-11. Equivalent model for the CIC decimation filter.
It is apparent that the amplitude response G f ( ) of the CIC filter is not
flat within the useful signal bandwidth, and therefore some compensation, by
means of a subsequent equalizer, is required in order to minimize signal
distortion. We also see that the particular value of the decimation factor U
determines the location of the frequency response’s nulls at the frequencies
/ mf m f d s U . Such nulls reveal crucial for rejecting those spectral
components that, owing to the decimation, are moved into the useful signal
baseband. The differential delay M causes the appearance of intermediate
nulls in between two adjacent nulls at mfd . These additional nulls are of
98 Chapter 3
little utility and do not significantly increase the alias rejection capability of
the CIC filter. This feature is highlighted in Figure 3-12, where the case
M =1 (dashed line) is compared with the case M =2 (solid thick line).
Actually, an increase of M does not yield any improvement in the rejection
of the unwanted spectral components, while it requires an increase in the
storage capability of the CIC filter. Therefore according to [Hog81] and
[Har97] we will restrict our attention in the sequel to the case M =1.
G(f)
f
fd 2fd Ufd=fs
fd/M
1
M=1
… fs/2
M=2
f '=0.455fs f "=0.545fs
Spectral Images from
Down-Conversion
BBB=0.1525fd
Useful
Signal
Spectrum
Spectral Images from
Decimation
Figure 3-12. Generic normalized frequency response of the CIC decimation filter.
The order N of the CIC filter determines the sharpness of the notches at
mfd and the amplitude of the relevant sidelobes, therefore it must be
carefully selected, taking into account the required attenuation of the
unwanted spectral components. Assuming that a white noise process is
superimposed on the signal at the CIC filter input, the shape of the frequency
response G f ( ) is proportional to the amplitude spectral density (i.e., the
square root of the power spectral density) of the noise process at the output
of the CIC, prior to decimation. Decimation causes the (normalized)
amplitude spectral density G f ( ) to be translated onto / mf m f d s U . As a
consequence the useful signal spectrum will suffer from aliasing caused by
the lobes of the spectral replicas, as clarified in Figure 3-13.
The total contribution of the aliasing spectral replicas, that we call alias
profile [Har97], is made of the contribution of U terms, and is bounded from
above by the function
2
2
0
d
k
k
A f G f kf
U
U
z
¦ . (3.39)
3. Design of an All Digital CDMA Receiver 99
The parameter N therefore keeps the alias profile A f ( ) as low as
possible within the useful signal’s bandwidth BBB .
Figure 3-14 shows the frequency response G f ( ) for the different
decimation ratios U in Table 3.2, for M 1, and N 4 , while Figure 3-15
reports G f ( ) for different orders of the filter N , for M 1, and U 8 . In
both the figures G f ( ) is plotted versus the normalized frequency / s f f .
G(f)
f
fd 2fd Ufd=fs
1
-2fd -fd … fs/2
BBB=0.1525fd
Useful
Signal
Spectrum
Aliases
Figure 3-13. Aliasing effect of the CIC filter caused by decimation.
As already mentioned, the spectrum of the signal at the output of the CIC
filter, at the decimated rate df , suffers from amplitude distortion, owing to
the non-constant frequency response H f ( ) (or, equivalently, G f ( )). This
calls for the use of a compensation filter (also termed equalizer) having a
frequency response ( ) H f eq given by
sin /
sin /
N
d
eq
d
f f H f Mf f
ª º S U « »
S ¬ ¼
(3.40)
such that
H fHf eq 1. (3.41)
We will consider the compensation filter ( ) G f eq for the normalized
frequency response G f ( ), that is