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put signal, the linearizer should have a
280 MHz VBW. This also implies that
the PA has a VBW high enough to al-
low the correction signal to be passed
to its output.
Squa re-cube Law Factor Dilemma
While being extremely simple, the
square-cube law has dramatic conse-
quences on all physics phenomena.
This law teaches that certain forces
will matter more or less depending on
the magnitude of a particular physics
quantity. What does this all have to do
with the topic? Take a 1 V sinusoid
and square it. This would be the sim-
plest way to generate the second har-
monic of the signal. The output signal
will be 1 V (see Figure 9). Now, do
the same thing with a 10 and 0.1 V
signal. The outputs will be 100 and
10 m V, respectively. In the fi rst case,
the output of the multiplier expanded
— 100 V > 1 V — and in the second,
the signal has been severely com-
pressed — 10 mV < 0.1 V.
What this means is that for ‘larger’
input signals, the polynomial genera-
tor output will be rapidly overwhelmed
while smaller signals will virtually
vanish. Solutions to the expansion
are two-fold: increasing the dynamic
range and increasing the resolution of
the coeffi cient DACs. The compres-
sion issue can only be resolved by am-
plifying the signal, that is adding gain.
A high gain can be achieved using a
cascade of amplifi cation stages with
the drawback that each stage requires
power and adds noise. Low noise am-
plifi cation is therefore a must.
Peak -to-Average Ratio Burden
The peak-to-average ratio (PAR)
is the ratio between the peak of the
signal and its average. In Figure 10,
a short time sample of a four carrier
W-CDMA signal with a 10 dB PAR
is shown. A single peak above 0.7 can
be seen, while most of the signal (the
average) is much lower. Multicarrier
applications, modern standards and
OFDM, in particular, lead to very high
PAR. What is important to understand
from a design standpoint is that the
analog circuits within the linearizer
basically have the same problem as the
PA. They have to support a high dy-
namic range to accommodate the PAR.
Worse, because the linearizer has to
create high order correction terms for
the polynomial, it will actually expand
be tightly controlled over process,
voltage and temperature (PVT). Only
a tight control will ensure that the per-
turbation energy is controlled.
DESI GN ISSUES EXPLAINED
Bandwidth Expansion
Predistortion is all about signal
expansion, hence bandwidth expan-
sion. For a given input signal at a fre-
quency f
0
, the PA will generate dis-
tortion products at multiples of this
frequency: 2f
0
, 3f
0
, 4f
0
, 5f
0
, 6f
0
, 7f
0
,
etc. While this is a good thing for a
rock guitar, modern telecommunica-
tion PA spectral output requirements
are very stringent and do not tolerate
too much distortion. The higher order
harmonics’ energy is high enough to
signifi cantly degrade the spectrum up
to the 7
th
order.
This means the linearizer should
be able to generate frequencies at
least up to 7f
0
to cancel this distortion
product at the output of the PA. In
other words, for a 40 MHz VBW in-
SPECIAL REPORT
68 MICROWAVE JOURNAL APRIL 2011
Fig. 9 Compression vs. expansion.
angle (rad)
max(sin(x)) = 10 V
max(sin(x)) = 1 V
sin(x) sin(x) * sin(x)
angle (rad)
max(sin(x)) = 0.1 V
angle (rad)
1
0
–1
0.1
0
–0.1
100
50
0
–50
1086420
1086420
67543210
AMPLITUDE (V)
AMPLITUDE (V)
AMPLITUDE (V)
Fig. 10 Peak to average ratio.
0.7
0.6
0.5
0.4
0.3
0.2
0.1
0
TIME 10
–3
4 CARRIERS W-CDMA, PAR = 9.99
5.545.505465.425.38
AMPLITUDE
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