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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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