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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 />

5 Quadrature method<br />

In the Quadrature System, two oscilla<strong>to</strong>rs at identical frequencies are used.<br />

One of the oscilla<strong>to</strong>rs will be the source being tested and the other will be a reference source<br />

whose performance is known <strong>to</strong> be better than the source under test. The sources are<br />

combined in a mixer and the resulting output signal is filtered and amplified by a Low <strong>Noise</strong><br />

Amplifier (LNA). A Fast Fourier Transform (FFT) Analyzer or a Spectrum Analyzer<br />

typically measures the output from the mixer.<br />

Source<br />

under<br />

test<br />

Mixer<br />

Reference<br />

source<br />

Low<br />

pass<br />

filter<br />

LNA<br />

Spectrum analyzer<br />

or<br />

FFT analyzer<br />

Figure 14: Block diagram of a phase noise measurement system using the Quadrature method<br />

The system behaves as a phase detec<strong>to</strong>r if the input signals <strong>to</strong> the mixer are adjusted <strong>to</strong> be in<br />

phase quadrature. When they are in quadrature the nominal DC output voltage from the mixer<br />

is 0 Volts. The output from the mixer is a direct measure of the phase difference between the<br />

two signals, and so it is also a direct measure of the phase noise of the UUT (assuming the<br />

reference source is better than the UUT).<br />

Setting the sources <strong>to</strong> be in phase quadrature is not always very easy. If both frequency<br />

sources are synthesizers with good long-term stability, then there is usually not a great<br />

problem. <strong>Phase</strong> quadrature can usually be achieved by offsetting the frequency of one of the<br />

sources, during which time the system will produce an AC voltage at the same frequency as<br />

the offset frequency, and then resetting the frequency <strong>to</strong> be the same. The synthesizers will<br />

settle <strong>to</strong> a new phase that can be checked <strong>to</strong> see if it is close enough <strong>to</strong> phase quadrature,<br />

typically a voltage less than 5% of the peak voltage from the phase detec<strong>to</strong>r when the<br />

frequencies are offset 9 . If one of the sources has fine frequency control (e.g. 0.1 Hz) the<br />

frequency can be set <strong>to</strong> a small offset and then returned <strong>to</strong> the required frequency when the<br />

correct phase is achieved. Alternatively, many modern synthesized sources include phase<br />

adjustment controls that can be used <strong>to</strong> adjust the phase more easily.<br />

However, in the many applications, measurements are undertaken under less than ideal<br />

conditions, and a feedback system has <strong>to</strong> be used <strong>to</strong> maintain phase quadrature. The feedback<br />

system forms a phase locked loop that controls the frequency/phase of one of the oscilla<strong>to</strong>rs <strong>to</strong><br />

9 This assumes the signal is larger than any residual offsets from the phase detec<strong>to</strong>r. More on this can be found in the section on measurement<br />

uncertainty.<br />

21

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