Agilent Spectrum Analysis Basics - Agilent Technologies
Agilent Spectrum Analysis Basics - Agilent Technologies
Agilent Spectrum Analysis Basics - Agilent Technologies
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Next let’s see to what extent harmonic mixing complicates the situation.<br />
Harmonic mixing comes about because the LO provides a high-level drive<br />
signal to the mixer for efficient mixing, and since the mixer is a non-linear<br />
device, it generates harmonics of the LO signal. Incoming signals can mix<br />
against LO harmonics, just as well as the fundamental, and any mixing<br />
product that equals the IF produces a response on the display. In other words,<br />
our tuning (mixing) equation now becomes:<br />
f sig = nf LO ±f IF<br />
where<br />
n = LO harmonic<br />
(Other parameters remain the same as previously discussed)<br />
Let’s add second-harmonic mixing to our graph in Figure 7-3 and see to what<br />
extent this complicates our measurement procedure. As before, we shall first<br />
plot the LO frequency against the signal frequency axis. Multiplying the<br />
LO frequency by two yields the upper dashed line of Figure 7-3. As we did<br />
for fundamental mixing, we simply subtract the IF (3.9 GHz) from and add<br />
it to the LO second-harmonic curve to produce the 2 – and 2 + tuning ranges.<br />
Since neither of these overlap the desired 1 – tuning range, we can again argue<br />
that they do not really complicate the measurement process. In other words,<br />
signals in the 1 – tuning range produce unique, unambiguous responses on<br />
our analyzer display. The same low-pass filter used in the fundamental mixing<br />
case works equally well for eliminating responses created in the harmonic<br />
mixing case.<br />
2+<br />
15<br />
2xLO<br />
Signal frequency (GHz)<br />
10<br />
5<br />
1+<br />
2–<br />
LO<br />
1–<br />
0<br />
4 5 6<br />
LO frequency (GHz)<br />
7<br />
Figure 7-3. Signals in the “1 minus” frequency range produce<br />
single, unambiguous responses in the low band, high IF case<br />
85