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Good Practice Guide to Phase Noise Measurement ... - Sequanux

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<strong>Measurement</strong> <strong>Good</strong> <strong>Practice</strong> <strong>Guide</strong> No. 68<br />

before being measured by the spectrum analyzer. The band-pass filter can be a commercially<br />

available induc<strong>to</strong>r/capaci<strong>to</strong>r, crystal or ceramic IF filter of the type commonly used in<br />

receiver systems. The filter needs <strong>to</strong> be able <strong>to</strong> reject the IF frequency but pass a selected<br />

band of noise <strong>to</strong> the spectrum analyzer. The filter needs <strong>to</strong> have a flat pass band response <strong>to</strong><br />

minimize the calibration problems that can be introduced. The spectrum analyzer filter<br />

bandwidth is set <strong>to</strong> be narrower than the band-pass filter and it is this filter that determines the<br />

bandwidth of the measurement.<br />

Source<br />

under<br />

test<br />

Mixer<br />

Low pass<br />

filter<br />

Xtal or ceramic<br />

filter<br />

Reference<br />

source<br />

Low noise<br />

amplifier<br />

Figure 11: <strong>Phase</strong> noise measurement using a down converter and a spectrum analyzer<br />

The improvement in performance using this method occurs because the carrier frequency is<br />

rejected at the IF output by the band-pass filter. The spectrum analyzer is being used <strong>to</strong><br />

measure a signal that is almost entirely consists of the signal that is being measured (the phase<br />

noise). <strong>Noise</strong> introduced by the mixing of the signal from the unit under test with the<br />

spectrum analyzer local oscilla<strong>to</strong>r is substantially reduced, as shown below, so the restrictions<br />

on measurement dynamic range are no longer critically dependent on the quality of the<br />

spectrum analyzer’s local oscilla<strong>to</strong>r. The dynamic range required of the spectrum analyzer is<br />

significantly reduced.<br />

Mix<br />

Amplify<br />

Filter<br />

1 GHz +10.7 MHz<br />

Mixer Input Signals<br />

10.7 MHz<br />

IF Output<br />

Measure on<br />

analyzer<br />

Figure 12: Frequency diagram for phase noise measurement using a down converter and a spectrum<br />

analyzer<br />

Some care needs <strong>to</strong> be taken in making measurements in this way. Suitable filters with<br />

narrow bandwidths are rarely designed for 50 ohm systems and often have severe changes of<br />

impedance with frequency. The mixer has <strong>to</strong> be buffered from this impedance variation <strong>to</strong><br />

avoid errors due <strong>to</strong> reflected signals re-mixing. The filters can also exhibit non-linear<br />

behavior at both low levels (particularly crystals) and high levels (as crystal or ceramic<br />

devices exceed their linear power ratings). These problems, combined with frequency<br />

response unflatness in the pass band, can make the measurement accuracy unreliable unless<br />

basic precautions are taken.<br />

The technique is also restricted <strong>to</strong> measurements at offsets of typically greater than 10 kHz<br />

since it relies on the filter having <strong>to</strong> reject a significant proportion of the carrier signal at the<br />

IF.<br />

15

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