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NIST Technical Note 1337: Characterization of Clocks and Oscillators

NIST Technical Note 1337: Characterization of Clocks and Oscillators

NIST Technical Note 1337: Characterization of Clocks and Oscillators

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ALLAN: PRECISiON CLOCKS AND OSCILLATORS-10-i5ACTIVE H MASERRb GAS cru,...........'.....---­-16:-_--;__---;.__--:-__-+-__--!-_~I 2 3 4 6lO:; TAU (s.econds)Fig. 10. Square root <strong>of</strong> Allan variance for variety <strong>of</strong> state-<strong>of</strong>-the-an precisionoscillators including NBS-6. NBS primary frequency st<strong>and</strong>ard.-6-7II'sRMS TIME DEVIATION&/~f7.//'Cs653minimum O',(T) value. We would then change the temperatureto the other value <strong>and</strong> repeat the measurementwith the same criteria <strong>and</strong> note the Ayr.. between the twooptimally detennined frequency values. If these two stepsare repeated several times, an arbitrarily good precisionfor the temperature coefficient is achieved if it is linear.The uncertainty is approximately given by (J,(7 )/JP,mwhere P is the number <strong>of</strong> Ayr.. values obtained fromswitching back <strong>and</strong> forth. Knowing the characteristics <strong>of</strong>both the r<strong>and</strong>om <strong>and</strong> the systematic deviations <strong>of</strong> precisionclocks <strong>and</strong> oscillators clearly is useful to the designer,the manufacturer, the planner, <strong>and</strong> the user as wellas the vendor <strong>of</strong> these devices.The aforementioned procedures usually work well if theclocks or oscillators are in a reasonable environment. Ifthe environment is adverse, other procedures <strong>and</strong> analysismethods may have to be employed. As a general rule it is<strong>of</strong>ten useful to analyze the data in the frequency domainas well as the time domain. The frequency domain is especiallyuseful if there are bright lines, i.e., sideb<strong>and</strong>s tothe carrier frequency, The effect <strong>of</strong> a modulation sideb<strong>and</strong>fm on 0', (7) can be calculated, <strong>and</strong> is given by [18](15)-130~=~-~--':-3----J4'---..,:---~---:!lOG TAU p (seconds)Fig. I I. From frequency stability characterization shown in Fig. 10, optimumprediction algorithms to minimize time error can be obtained.Based on oplimum prediction procedures rms time prediclion error forprediction inlerval T p can be calculated for each oscillator shown in Fig.10 <strong>and</strong> corresponding values are plotted in Fig. II.state-<strong>of</strong>-the-art oscillators, <strong>and</strong> Fig. 11 shows the nns timeprediction errors for the same set <strong>of</strong> oscillators.CONCLUSIONIn conclusion, it is clear that classical statistics do notallow characterization <strong>of</strong> common kinds <strong>of</strong> r<strong>and</strong>om signalvariations found in precision oscillators. The two-sampleAllan variance provides a valuable <strong>and</strong> convergent measure<strong>of</strong> the power-law spectral-density models useful incharacterizing r<strong>and</strong>om deviations for most oscillators <strong>and</strong>clocks, Once characterized, we can calculate optimumtime <strong>and</strong> frequency estimates as well as predicted values.Characterizing the r<strong>and</strong>om variations also provides nearoptimumestimation <strong>of</strong> systematic effects, which <strong>of</strong>tencause the predominant time <strong>and</strong> frequency deviations. ForeX:lmple, if we wanted to optimally detennine the statictemperature dependence with the temperature set at twodifferent values, we would stabilize the oscillator at onetemperature <strong>and</strong> measure the frequency against a referencefor a time T"'" corresponding to the T for the nominalwhere x pp is equal to the peak-to-peak or twice the amplitude<strong>of</strong> the time-deviation modulation.If one is trying to estimate the power-law spectral behaviorbetween a pair <strong>of</strong> oscillators or clocks using O'y (7),it is apparent from (15) that if significant modulationsideb<strong>and</strong>s are present on the signal, these can seriouslycontaminate that estimate. However, if a O"y( 7) plot displaysa character as given by (15), then the amplitude <strong>and</strong>frequency <strong>of</strong> that modulation sideb<strong>and</strong> can be estimatedfrom this time-domain analysis technique. In practice, thisapproach is <strong>of</strong>ten used, but these modulation sideb<strong>and</strong>scan be more efficiently estimated in the frequency domain.If the measurement sampling rate 1/70 is set equalto 1m' then the modulation sideb<strong>and</strong> is aliased away <strong>and</strong>has no effect on l1y ( 7).The best rule in all analysis is to use common sense.Very <strong>of</strong>ten the most revealing information may be in aplot <strong>of</strong> the raw time (phase) difference or frequency-differenceresiduals after some trend has been removed. Sucha plot is usually the first thing to look at when characterizingclocks <strong>and</strong> oscillators. Caution here 'is also importantas a pure r<strong>and</strong>om walk on the time residuals (whiteFM) may be visually interpreted as having frequencysteps. This is especially true for flicker FM as <strong>of</strong>ten seenin quartz-crystal oscillators. Following the time-residualplot with a l1 y ( 7) analysis <strong>of</strong>ten answers the question asto whether or not such steps are statistically significant.ACKNOWLEDGMENTBecause the paper is mainly a review, the author is indebtedto a large number <strong>of</strong> people-many <strong>of</strong> whom arereflected in the references. Specifically. sincere appreciationis expressed to Dr. James A. Barnes, Mr. Dick D.IN-127

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