ADL5593 [ADI]

Correcting Imperfections in IQ Modulators to Improve RF Signal Fidelity; 校正IQ调制器缺陷,提高射频信号保真度
ADL5593
型号: ADL5593
厂家: ADI    ADI
描述:

Correcting Imperfections in IQ Modulators to Improve RF Signal Fidelity
校正IQ调制器缺陷,提高射频信号保真度

射频
文件: 总8页 (文件大小:209K)
中文:  中文翻译
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AN-1039  
APPLICATION NOTE  
One Technology Way • P. O. Box 9106 • Norwood, MA 02062-9106, U.S.A. • Tel: 781.329.4700 • Fax: 781.461.3113 • www.analog.com  
Correcting Imperfections in IQ Modulators to Improve RF Signal Fidelity  
by Eamon Nash  
changes, in-factory and in-field algorithms that can reduce the  
effect of these modulator imperfections is also discussed, and  
particular focus is placed on the efficacy of in-factory set-and-  
forget algorithms.  
INTRODUCTION  
The in-phase and quadrature modulator (IQ modulator) is a  
key component in modern wireless transmitters. It provides a  
convenient method for modulating data bits or symbols onto  
an RF carrier. IQ upconversion has become the architecture  
of choice for implementing transmitter signal chains for end  
applications such as cellular, WiMAX, and wireless point-to-  
point. IQ modulators, however, can degrade signal fidelity in  
ways that are somewhat unique. These effects can degrade the  
quality of the transmitted signal during the modulation process,  
resulting in degraded error vector magnitude (EVM) at the  
receiver, which in turn degrades bit error rate (BER). Fortu-  
nately, algorithms exist that can correct these imperfections.  
A TYPICAL WIRELESS TRANSMITTER  
Figure 1 shows a block diagram of a direct-conversion wireless  
transmitter that uses an IQ modulator to modulate a bit stream  
onto a carrier. A single bit stream is split into two parallel bit  
streams at half the original data rate. To limit the spectral band-  
width of the final carrier, the two bit streams are low-pass filtered  
in the digital domain. To do this, the original bit-streams must  
be digitally oversampled by the digital signal processor or field  
programmable gate array (FPGA). So, instead of two bit streams,  
there are now two streams of digital words. The chosen resolu-  
tion of these words depends upon multiple factors such as the  
required signal-to-noise ratio of the link and the chosen mod-  
ulation scheme (QPSK in this case). Word widths between 12  
and 16 bits are commonly chosen.  
This application note describes a typical zero-IF or direct-  
conversion transmitter and provides a brief introduction to  
digital modulation. Other items discussed are: the imper-  
fections introduced by the modulator are examined with  
particular focus on the effect of temperature and frequency  
Q
AD9788  
FPGA OR DSP  
I
AUX  
DAC1  
GAIN  
DAC 1  
ADL5375  
100  
800  
600  
OVERSAMPLE  
LOW-PASS  
FILTER  
LOW-  
PASS  
FILTER  
DIGITAL  
FILTER  
PHASE  
ADJUST  
16-BIT  
I DAC  
400  
200  
0
–200  
–400  
–600  
–800  
800  
600  
400  
200  
50Ω  
0
–200  
–400  
–600  
–800  
HPA  
ADL5320  
0°  
800  
600  
400  
200  
0
90°  
–200  
–400  
–600  
–800  
800  
600  
AUX  
DAC2  
LOW-  
PASS  
FILTER  
1.0  
1.5  
2.0  
400  
TIME (msec)  
200  
0
AD8363  
–200  
–400  
–600  
–800  
100Ω  
50dB RMS  
800  
600  
400  
200  
GAIN  
DAC 2  
DETECTOR  
1.329  
1.829  
2.329  
TIME (msec)  
0
–200  
–400  
–600  
–800  
OVERSAMPLE  
LOW-PASS  
FILTER  
DIGITAL  
FILTER  
PHASE  
ADJUST  
16-BIT  
Q DAC  
1.0  
1.5  
TIME (msec)  
2.0  
50Ω  
SPECTRUM  
ANALYZER  
DIGITAL  
DEMOD  
AD9230  
AD8352  
Figure 1. A Zero IF Direct-Conversion Transmitter with Optional Loop-Back Receiver  
Rev. 0 | Page 1 of 8  
 
 
AN-1039  
Application Note  
TABLE OF CONTENTS  
Introduction ...................................................................................... 1  
Correcting for Quadrature and I/Q Gain Errors ......................6  
Frequency Variations ....................................................................7  
Post Calibration Temperature Drift............................................7  
Calibration vs. Time......................................................................7  
Complex Modulation....................................................................8  
Conclusions....................................................................................8  
A Typical Wireless Transmitter ...................................................... 1  
Modulator Imperfections ............................................................ 3  
Correcting Modulator Imperfections ........................................ 4  
Factory Calibration ...................................................................... 4  
Calibration Procedure.................................................................. 6  
Rev. 0 | Page 2 of 8  
Application Note  
AN-1039  
After low-pass filtering, the two word streams are applied to a  
pair of digital-to-analog converters (DAC). The DAC outputs  
drive two low-pass filters whose primary role is to remove  
Nyquist images. The outputs of these filters then drive the  
baseband inputs of the IQ modulator. The local oscillator (LO)  
input of the modulator is driven by a relatively pure CW signal  
generated by a phase-locked loop (PLL) such as the ADF4106  
from Analog Devices, Inc. Now, take a closer look at the  
operation of the IQ modulator.  
MODULATOR IMPERFECTIONS  
Contrary to the previous hypothetical situation, in a real IQ  
modulator, things do not look so perfect. A series of effects in  
the IQ modulator conspire to create QPSK (or QAM) vectors  
that are neither equal in amplitude nor separated by exactly 45°.  
Consider first what happens if for some reason the gain of the I  
path is greater than that of the Q channel; this could be caused  
by a DAC gain mismatch, low-pass filter insertion loss, mismatch,  
or gain imbalance inside the IQ modulator. Regardless of where  
this gain imbalance comes from, its effect is the same. Because  
the 0°/180° vectors at the output of the I multiplier are larger  
than the +90°/−90° vectors from the Q multiplier, the shape  
of the constellation becomes rectangular (see Figure 2B). This  
degrades signal integrity at the receiver because the receiver is  
expecting a perfectly square constellation. In the QPSK example  
shown in Figure 2B, a slight gain imbalance is unlikely to result  
in an incorrect bit decision in the receiver unless the received  
signal is very small. However, in higher order modulation  
schemes such as 16 QAM or 64 QAM (see Figure 2E and  
Figure 2F), the increased density of the constellation points  
could easily combine with an IQ gain imbalance to produce  
an incorrect symbol decision in the receiver.  
The LO signal is split into two signals, equal in amplitude but  
with a phase difference of exactly 90°. These two quadrature  
signals drive the inputs of the two mixers that, for the purposes  
of this application note, are viewed as analog multipliers. The  
outputs of these two multipliers are added together (in the  
Σ block of the IQ modulator) to provide the IQ modulators  
output.  
While it is apparent that the baseband data streams have  
been filtered, instead briefly consider them as the original bit  
streams. Instead of a stream of 1s and 0s, think of them as two  
streams switching between a value of +1 and –1. So, the output  
of the I multiplier consists of a vector which is flipping in-phase  
between 0° and 180°as the bit stream alternates. Likewise, the  
output of the Q multiplier is a vector that flips between +90°  
and –90° as the bit stream modulates the original 90° vector.  
Thus, if at a particular instant, both the I and Q bit streams are  
equal to +1, the result at the output of the IQ modulator is the  
sum of the 90° and 0° vectors, that is, a +45° vector. Likewise,  
I and Q bit combinations of −1/+1, −1/−1, and +1/−1 produce  
vectors (commonly called symbols) all of equal amplitude at  
+135°, −135°, and −45°, respectively. If these vectors were  
plotted, observe the constellation of the modulated carrier  
(see Figure 2A).  
In most IQ modulators, the 90° phase split of the LO is achieved  
using either a polyphase filter or a divide-by-two flip-flop circuit  
(which requires an external LO that is twice the desired output  
frequency). In either circuit, the 90° phase split or quadrature is  
never perfect. For example, if there is a 1° quadrature error, the  
shape of the resulting constellation is slightly trapezoidal (see  
Figure 2C). Just like IQ gain imbalance, this can result in  
incorrect bit decisions in the receiver.  
Now consider what happens if either the I or Q paths have  
unwanted dc offset errors. This results in the +1/−1 multipli-  
cation being skewed. For example, an offset that is equal to 1%  
of the baseband signal amplitude causes the +1/−1 multipliers  
to be modified to +1.01/−0.99. This has the effect of shifting  
the center of the constellation off the origin, on either the I or  
Q axis, most likely in both (see Figure 2D). In the frequency  
domain, this manifests itself as a small portion of the unmodu-  
lated carrier appearing at the output of the modulator. In the  
frequency domain, this LO leakage (also referred to as LO  
feedthrough) appears at the center of the modulated spectrum.  
(A)  
(B)  
(C)  
Because of parasitic capacitances within the silicon die and  
bond-wire to bond-wire coupling, the signal that is applied  
to the LO port of the IQ modulator may also couple directly  
to the RF output. This leakage is independent of the offset  
multiplication effect that was described previously. However,  
its manifestation, that is, the presence of the unmodulated  
carrier in the output spectrum, is exactly the same. Thus, the  
net LO leakage seen at the output of the IQ modulator is the  
vector sum of these two components. Fortunately, as discussed  
in the Correcting Modulator Imperfections section, the com-  
posite LO leakage at the output can be mitigated by a single  
compensation technique.  
(D)  
(E)  
(F)  
Figure 2. Error Vector Magnitude Constellations that Result from Various  
Modulator Imperfections  
Rev. 0 | Page 3 of 8  
 
 
AN-1039  
Application Note  
Table 1. IQ Modulator Selection Table Showing Uncompensated Gain and Phase Imbalance  
IQ 3dB  
CARRIER  
SIDEBAND  
GAIN  
PHASE  
NOISE  
SUPPLY  
SUPPLY  
PART  
NUMBER  
FREQUENCY BANDWIDTH SUPPRESS SUPPRESSION IMBALANCE IMBALANCE  
FLOOR  
P1dB  
OUTPUT  
VOLTAGE  
(V)  
CURRENT SPECS @  
(MHz)  
(MHz)  
(dBm)  
(dBc)  
(dB)  
(°)  
(dBm/Hz) (dBm) IP3 (dBm)  
(mA)  
(MHz)  
AD8345  
AD8346  
AD8349  
140 TO 1000  
800 TO 2500  
700 TO 2700  
0.50  
1.00  
2.70 TO 5.50  
2.70 TO 5.50  
4.75 TO 5.50  
4.75 TO 5.25  
4.75 TO 5.25  
4.75 TO 5.25  
4.75 TO 5.25  
4.75 TO 5.25  
4.75 TO 5.25  
4.75 TO 5.50  
4.75 TO 5.50  
4.75 TO 5.50  
4.75 TO 5.50  
65  
45  
800  
1900  
900  
80  
–42  
–42  
–45  
–50  
–50  
–45  
–32  
–33  
–46  
–46  
–38  
–44  
–39  
–42  
–36  
–35  
–41  
–55  
–45  
–57  
–50  
–52  
–50  
–46  
–50  
–48  
0.200  
0.200  
0.100  
0.030  
0.100  
0.090  
0.010  
0.015  
–0.050  
–0.030  
0.050  
0.050  
0.050  
–155.0  
–147.0  
–155.0  
–160.0  
–158.6  
–158.0  
–157.0  
–160.0  
–160.0  
–159.0  
–160.0  
–157.0  
–157.0  
2.5  
–3.0  
7.6  
N/A  
N/A  
70  
1.90  
21.0  
24.0  
27.0  
27.0  
26.0  
22.8  
27.0  
26.0  
25.0  
29.0  
30.0  
135  
205  
175  
165  
174  
173  
200  
215  
230  
170  
170  
160  
500  
500  
500  
500  
500  
750  
700  
700  
250  
250  
ADL5370 300 TO 1000  
ADL5371 500 TO 1500  
ADL5372 1500 TO 2500  
ADL5373 2300 TO 3000  
ADL5374 3000 TO 4000  
ADL5375 400 TO 6000  
ADL5385 50 TO 2200  
ADL5386 50 TO 2200  
ADL5590 869 TO 960  
ADL5591 1805 TO 1990  
11.0  
14.4  
14.2  
13.8  
12.0  
9.4  
450  
0.76  
900  
–0.03  
0.21  
1900  
2500  
3500  
900  
0.10  
0.25  
–0.29  
–0.39  
–0.50  
0.20  
11.0  
11.1  
16.0  
16.0  
350  
350  
940  
1960  
0.30  
CORRECTING MODULATOR IMPERFECTIONS  
FACTORY CALIBRATION  
Note that in Figure 1, in addition to the direct conversion signal  
chain, an optional loop-back or transmit observation receiver  
has also been incorporated into the radio. The primary function  
of this receiver is to analyze the adjacent channel power ratio  
(ACPR) of the transmitter that is primarily caused by distortion  
in the high power amplifier (HPA). By continually observing  
the ACPR of the transmitter, digital predistortion of the  
baseband signal can be employed to partially correct HPA  
nonlinearities while allowing the HPA to operate closer to its  
compression point.  
If a wireless transmitter does not use digital predistortion, it  
would be difficult to justify the cost of a loop-back receiver  
purely for the sake of the IQ modulator. In such situations,  
the two options that remain are:  
Do not perform any correction of the IQ modulators  
imperfections.  
Complete a one-time factory calibration and store the  
correction coefficients in nonvolatile memory.  
In recent years, the performance of IQ modulators has  
improved to such a degree that it is now feasible (depending  
on the modulation scheme) to design a transmitter without any  
need to provide correction for imperfections. For example, the  
ADL5375 from Analog Devices has gain and quadrature imbal-  
ances of 0.05 dB and 0.29°, respectively, at 900 MHz, with little  
or no degradation over temperature. As a result, in many appli-  
cations, it may be adequate to dispense with any correction  
algorithms. Table 1 shows the performance of this and other  
members of the Analog Devices IQ modulator family.  
The presence of a loop-back receiver can be opportunistically  
used to also correct for modulator imperfections.  
A detailed discussion of the IQ modulator correction tech-  
niques used when a loop-back receiver is present is beyond the  
scope of this application note. However, the general procedure  
involves using the loop-back receiver to demodulate the I and  
Q bit streams. The demodulated constellation is then examined  
for evidence of IQ gain imbalance, imperfect quadrature, and/  
or LO leakage. Once these imperfections have been identified,  
the I and Q data streams can be preprocessed so that the IQ  
modulator imperfections cancel out. For example, if the  
demodulated constellation from the loop-back receiver shows  
a rectangular constellation with the width of I being larger than  
the height of Q (see Figure 2B), gain adjust registers in the DAC  
can be used to either decrease the size of the I data stream or  
increase the size of the Q data stream. Likewise, the phase  
adjustment registers of the DAC can be used to slightly skew  
the I and Q channels so that the imperfect quadrature of the  
IQ modulators phase splitter is compensated.  
Rev. 0 | Page 4 of 8  
 
 
Application Note  
AN-1039  
The second alternative presented previously is to perform  
factory calibration. To do this, the popular single sideband  
spectrum can be used as a simple but valuable diagnosis  
tool during factory calibration. To create a single sideband  
spectrum, the I and Q inputs are driven by low frequency  
(typically 1 MHz) sine and cosine signals, that is, the base-  
band signals are in quadrature. Figure 3 shows the spectrum  
that results when these baseband signals are mixed with the LO.  
The primary components of the single sideband spectrum are:  
Figure 4 shows a plot that can be used to relate sideband  
suppression to I/Q gain mismatch and quadrature mismatch.  
From the plot, it can be noted that a quadrature phase error of  
1°, coupled with an I/Q gain mismatch of 0.5 dB, results in  
−30 dB of sideband suppression. It is notable in this example  
that improving the quadrature phase mismatch has no effect  
on the sideband suppression unless the gain mismatch is also  
improved.  
0
–10  
Lower sideband: If the IQ modulator has no imperfections,  
this is the only spectral component observed, the result of  
multiplication and summing of the baseband sine and  
cosine signals with the two in-quadrature LO signals.  
Undesired upper sideband: This undesired component  
results from gain and phase imbalances between the I and  
Q signal paths along with LO quadrature imbalance.  
Undesired LO leakage: As discussed earlier, the LO leakage  
results from I and Q offsets and/or parasitic leakage of the  
LO directly to the IQ modulators output.  
2.5dB  
–20  
1.25dB  
0.5dB  
–30  
–40  
–50  
–60  
–70  
–80  
0.25dB  
0.125dB  
0.05dB  
0.025dB  
0.0125dB  
0dB  
–90  
0
–10  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
–90  
0.01  
0.1  
1
10  
100  
PHASE ERROR (Degrees)  
Figure 4. Plot Showing the Relationship Between Modulator Errors and  
Sideband Suppression  
By using a directional coupler and a power splitter (as shown  
in Figure 1), it is quite simple to add an auxiliary output to  
the transmitter that can be used during factory calibration. A  
spectrum analyzer is connected to this port. Another alternative  
would be to connect the spectrum analyzer at the antenna  
connector (after the signal has been adequately attenuated).  
CENTER 899.9334MHz  
333kHz/  
SPAN 3.33MHz  
Figure 3. Single Sideband Spectrum  
Rev. 0 | Page 5 of 8  
 
 
AN-1039  
Application Note  
CALIBRATION PROCEDURE  
CORRECTING FOR QUADRATURE AND I/Q GAIN  
ERRORS  
Correcting all of the modulator’s imperfections is a multistep  
process. Start by looking at the procedure for LO leakage cor-  
rection which results in a constellation that is offset from the  
origin. A single sideband spectrum is applied to the transmitter  
and is monitored on the spectrum analyzer. Next, small diffe-  
rential offset voltages are applied to the I and Q inputs. Applying  
differential offset voltages to the I and Q inputs should not be  
confused with changing the dc bias levels (also referred to as the  
common-mode level) on these pins, which has no effect. This is  
done as an I offset sweep followed by a Q offset sweep (or vice  
versa). Returning briefly to Figure 1, note that the AD9788 (a  
16-bit, 800 MSPS dual DAC) conveniently includes two aux-  
iliary DACs that can be used to couple differential dc offset  
voltages on I and Q lines. This coupling is performed externally  
using resistor dividers.  
A similar procedure can be used to correct quadrature and I/Q  
gain mismatch. IQ modulator family data sheets typically specify  
the quadrature phase mismatch and I/Q gain imbalance in  
degrees and decibels, respectively, along with the sideband  
suppression (also in decibels). Using this information, it is  
advisable to perform the first optimization pass on the weaker  
of the two specifications, that is, the specification which most  
contributes to the sideband suppression. For example, assume  
that the device data sheet specifies a sideband suppression of  
−40 dBc, comprising of 1 degree of phase imbalance and 0.1 dB  
of gain imbalance amplitude. In this case, it is advisable to first  
try to adjust phase because making a gain adjustment has  
almost no effect as long as the 1 degree of phase error is present  
(see Figure 4).  
Figure 5 shows how sweeping the I and Q offset voltages alters  
the LO leakage. Start by sweeping the I offset voltage around 0 V  
while holding the Q offset voltage at 0 V. With modern IQ  
modulators exhibiting unadjusted LO leakage in the −40 dBm  
range and having voltage gains in the −5 dB to +5 dB range, an  
offset voltage sweep range of 5 mV is more than adequate to  
identify the location of the null (in this example, 2 mV is  
adequate to identify a nulling voltage somewhere between  
100 μV and 200 μV). Note, however, that the first pass (black  
trace) only manages to reduce the LO leakage to just under  
−40 dBm. This clearly indicates that the Q offset needs  
correction. The second pass (blue trace) involves sweeping  
the Q offset around 0 V with the I offset held at the value that  
yielded the first I null. Note that a Q offset of 400 μV reduces  
the LO leakage a further 10 dB to around −50 dBm. However,  
a third pass is required. The trough from the first pass is quite  
shallow because the Q channel had not yet been adjusted. This  
makes it difficult to identify the ideal I nulling voltage. A third  
pass (red trace) that involves again sweeping the I offset while  
holding the Q offset at 400 μV, identifies the optimum I nulling  
voltage to be 150 μV.  
Figure 6 shows the results of a gain sweep followed by a  
phase sweep. In the first pass, the gain delta between I and Q  
is adjusted over a range of approximately 2 dB. The TxDAC®  
in Figure 1 facilitates this adjustment by providing internal  
gain adjust auxiliary DACs. The sweep yields a null of around  
−57 dBc for a gain difference of approximately −0.1 dB (gain is  
scaled on the top axis). Next, adjust the skew between I and Q.  
This drives the null down further to −60 dBc for a phase adjust  
of −0.05°.  
GAIN ADJUST (dB)  
–2  
–10  
–1  
0
1
2
–20  
–30  
–40  
–50  
–60  
–70  
FIRST PASS (GAIN ADJUST)  
SECOND PASS (PHASE ADJUST)  
0
–10  
–20  
–30  
–40  
–50  
–60  
–70  
–80  
FIRST PASS – I OFFSET ADJUST  
SECOND PASS – Q OFFSET ADJUST  
THIRD PASS – I OFFSET ADJUST  
–0.4  
–0.3  
–0.2  
–0.1  
0
0.1  
0.2  
0.3  
0.4  
PHASE ADJUST (Degrees)  
Figure 6. Multipass Sideband Suppression Compensation Sweeps  
In this case, a third pass is not necessary and does not yield  
further improvement. This stems from the fact that the  
unadjusted phase error is very close to the optimized value  
(~0.05°). Thus, the first-pass gain adjust yields a deep trough  
that is only slightly improved during the phase sweep. This  
contrasts to the LO leakage nulling where a third pass yielded  
further improvement.  
–2  
–1  
0
1
2
I AND Q DIFFERENTIAL OFFSET VOLTAGES (mV)  
Figure 5. Multipass LO Leakage Compensation Sweeps  
Rev. 0 | Page 6 of 8  
 
 
 
Application Note  
AN-1039  
Once the LO leakage and quadrature error have been calibrated,  
all that remains is for the calibration coefficients to be stored in  
nonvolatile RAM so that they are available when the equipment  
is turned on in the field. To recap, the four calibration  
coefficients are  
POST CALIBRATION TEMPERATURE DRIFT  
Factory calibration at multiple temperatures is even more  
difficult and expensive than calibration at multiple frequencies.  
As a result, it is generally only practical to perform factory  
adjustment of LO leakage and sideband suppression at an  
ambient temperature. Thus, what happens to post-calibration  
performance as temperature varies?  
I channel offset voltage  
Q channel offset voltage  
I channel vs. Q channel gain imbalance  
Quadrature phase imbalance  
In Figure 8, the LO leakage and sideband suppression have  
again been nulled midband. After nulling, the device is cycled  
over temperature. This again has the effect of moving sideband  
suppression and LO leakage off their nulled levels. However,  
notice that the performance at temperature is quite flat across  
frequency and it is no longer clear at which frequency the  
nulling was performed. The net improvement over temperature  
is approximately 15 dB compared to the unadjusted LO leakage.  
FREQUENCY VARIATIONS  
Calibrating at multiple frequencies within a band adds time to  
the factory calibration, requires more nonvolatile memory for  
the larger look up table, and is more cumbersome during field  
operation as calibration coefficients have to be swapped out as  
the frequency changes.  
CALIBRATION VS. TIME  
Now, consider what happens to the quality of calibration as the  
frequency changes. In Figure 7, sideband suppression and LO  
leakage have been nulled to −60 dBc and −74 dBm, respectively,  
at 1900 MHz. Figure 7 also shows how the uncompensated  
sideband suppression and LO leakage vary with frequency (the  
flatter green and red traces a the top of the plot). Next, adjust  
the frequency over a range of 30 MHz (the typical width of a  
cellular telephony band) without recalibration. The LO leakage  
quickly loses its null and at some frequencies is only around  
8 dB better than the uncompensated value. In the case of the  
sideband suppression, the difference between the compensated  
and uncompensated values becomes as low as around 1 dB.  
Figure 7 suggests that factory calibration be performed at  
multiple frequencies within a band to maintain nulled  
performance across the band.  
In the set-and-forget factory calibration scheme that has just  
been described, the question of long-term drift arises because  
the equipment may never be recalibrated in the field. Experi-  
ments have shown that it is very difficult, if not impossible, to  
measure the degradation of nulled sideband suppression and  
LO leakage over time. Very mild changes in environmental  
conditions tend to quickly move the device off its null. This  
makes it impossible to determine whether the environment and  
the test equipment are altering the experiment or if genuine  
device drift over time is taking place.  
However, Figure 8 shows that the question of drift over time  
is less important. This is because the effect of temperature drift  
is much more significant. Thus, in a system that experiences  
reasonable temperature fluctuations, whatever drift over time  
takes place is completely masked by the temperature drift.  
–30  
–30  
UNADJUSTED SIDEBAND SUPPRESSION (dBc)  
–35  
UNADJUSTED LO LEAKAGE (dBm)  
–35  
–40  
–45  
–50  
–55  
–60  
–40  
–45  
–50  
–55  
–60  
–65  
–65  
POST (MIDBAND)  
NULLING SIDEBAND  
SUPPRESSION (dBc)  
–70  
–75  
–80  
+25°C UNADJUSTED  
+25°C NULLED  
+85°C UNADJUSTED  
+85°C NULLED  
–40°C UNADJUSTED  
–70  
POST (MIDBAND) NULLING LO LEAKAGE (dBm)  
–75  
–40°C NULLED  
1870  
1880  
1890  
1900  
1910  
1920  
1930  
–80  
1802  
OUTPUT FREQUENCY (MHz)  
1812  
1822  
1832  
1842  
1852  
1862  
1872  
1882  
LO FREQUENCY (MHz)  
Figure 7. Variation of LO Leakage and Sideband Suppression vs. Frequency  
after Nulling Midband  
Figure 8. Variation of LO Leakage vs. Frequency and Temperature After  
Nulling Midband  
Rev. 0 | Page 7 of 8  
 
 
 
 
 
AN-1039  
Application Note  
COMPLEX MODULATION  
CONCLUSIONS  
While a detailed discussion is beyond the scope of this article,  
it is worth mentioning that all of the issues associated with  
modulator imperfections can be avoided with a slightly differ-  
ent transmit architecture. Many modern DACs incorporate  
complex modulators, that is, digital engines that convert  
baseband I and Q data up to a low intermediate frequency (IF).  
These signals, which are still in Cartesian I and Q format, drive  
the IQ modulator. Because modern IQ modulators, such as  
the ADL5375, have baseband input bandwidths of as high as  
750 MHz, low IFs in the 100 MHz to 250 MHz range can be  
easily accommodated. When an IQ modulator is driven by  
such a signal, the output spectrum is essentially a single  
sideband spectrum similar to what is shown in Figure 3.  
While modern IQ modulators offer excellent out-of-the-box  
quadrature accuracy, IQ gain imbalance, and LO leakage, their  
performance can be improved further using calibration. If the  
transmitter incorporates a loop-back receiver as part of a digital  
predistortion scheme, the receiver can also be used to conti-  
nuously monitor and correct the imperfections of the IQ  
modulator. The post-calibration performance is only limited  
by the available compensation step sizes and the ability of the  
receiver to precisely measure the constellation degradation.  
In transmitters that do not contain a loop-back receiver, factory  
calibration is a reasonable alternative. A single calibration in the  
middle of a operating band most likely causes degradation at  
the band edges. As a result, calibration at multiple frequencies  
within a band is more effective. When temperature drift is  
factored in, factory calibration at the ambient temperature  
typically improves LO leakage and sideband suppression by  
around 10 dB to 15 dB.  
The lower sideband becomes the modulated carrier and is  
displaced from the LO by a frequency offset equal to the  
intermediate frequency. The imperfections of the IQ modulator  
now manifest themselves as out-of-band effects, which can be  
filtered away, resulting in in-band EVM, which is not affected  
by the IQ modulator’s imperfections.  
However, this approach comes at some cost. Care must be taken  
to filter out the LO leakage along with the undesired upper  
sideband. In contrast, a Nyquist filtered zero IF spectrum is  
completely free of spurious components apart from harmonics  
of the LO. In addition, as the frequency of the low IF increases,  
the distortion of the DAC and IQ modulator increases slightly.  
©2009 Analog Devices, Inc. All rights reserved. Trademarks and  
registered trademarks are the property of their respective owners.  
AN08383-0-10/09(0)  
Rev. 0 | Page 8 of 8  
 

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