Agilent Spectrum Analysis Basics - Agilent Technologies
Agilent Spectrum Analysis Basics - Agilent Technologies
Agilent Spectrum Analysis Basics - Agilent Technologies
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Pluses and minuses of preselection<br />
We have seen the pluses of preselection: simpler analyzer operation,<br />
uncluttered displays, improved dynamic range, and wide spans. But there<br />
are some minuses, relative to an unpreselected analyzer, as well.<br />
First of all, the preselector has insertion loss, typically 6 to 8 dB. This loss<br />
comes prior to the first stage of gain, so system sensitivity is degraded by the<br />
full loss. In addition, when a preselector is connected directly to a mixer, the<br />
interaction of the mismatch of the preselector with that of the input mixer<br />
can cause a degradation of frequency response. Proper calibration techniques<br />
must be used to compensate for this ripple. Another approach to minimize<br />
this interaction would be to insert a matching pad (fixed attenuator) or<br />
isolator between the preselector and mixer. In this case, sensitivity would<br />
be degraded by the full value of the pad or isolator.<br />
Some spectrum analyzer architectures eliminate the need for the matching<br />
pad or isolator. As the electrical length between the preselector and mixer<br />
increases, the rate of change of phase of the reflected and re-reflected signals<br />
becomes more rapid for a given change in input frequency. The result is a<br />
more exaggerated ripple effect on flatness. Architectures such as those used<br />
in the ESA Series and PSA Series include the mixer diodes as an integral<br />
part of the preselector/mixer assembly. In such an assembly, there is minimal<br />
electrical length between the preselector and mixer. This architecture thus<br />
removes the ripple effect on frequency response and improves sensitivity by<br />
eliminating the matching pad or isolator.<br />
Even aside from its interaction with the mixer, a preselector causes some<br />
degradation of frequency response. The preselector filter pass band is<br />
never perfectly flat, but rather exhibits a certain amount of ripple. In most<br />
configurations, the tuning ramp for the preselector and local oscillator come<br />
from the same source, but there is no feedback mechanism to ensure that<br />
the preselector exactly tracks the tuning of the analyzer. Another source<br />
of post-tuning drift is the self-heating caused by current flowing in the<br />
preselector circuitry. The center of the preselector passband will depend<br />
on its temperature and temperature gradients. These will depend on the<br />
history of the preselector tuning. As a result, the best flatness is obtained<br />
by centering the preselector at each signal. The centering function is typically<br />
built into the spectrum analyzer firmware and selected either by a front panel<br />
key in manual measurement applications, or programmatically in automated<br />
test systems. When activated, the centering function adjusts the preselector<br />
tuning DAC to center the preselector pass band on the signal. The frequency<br />
response specification for most microwave analyzers only applies after<br />
centering the preselector, and it is generally a best practice to perform this<br />
function (to mitigate the effects of post-tuning drift) before making amplitude<br />
measurements of microwave signals.<br />
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