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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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12 FREQUENCY AND TIME MEASUREMENTI~I----.------;-----+­211TIMEFIG.12-11 Calculation <strong>of</strong> two average frequencies.vl <strong>and</strong> Yz by measuring the phase <strong>of</strong> anoscillator x(/) at times I,. t 2 • <strong>and</strong> r l .completely symmetric, with negative values being as likely as positive ones.The resulting distribution is called a chi-squared distribution, <strong>and</strong> it has one"degree <strong>of</strong> freedom" since the distribution was obtained by considering thesquares <strong>of</strong> individual (i.e., one independent sample), normally distributedvariables (Jenkins <strong>and</strong> Watts, 1968).In contrast, from five phase values four consecutive frequency values canbe calculated, as shown in Fig. 12-12. It is possible to take the first pair <strong>and</strong>calculate a sample Allan variance. A second sample Allan variance can becalculated from the second pair (i.e., the third <strong>and</strong> fourth frequencymeasurements). The average <strong>of</strong> these two sample Allan variances provides animproved estimate <strong>of</strong> the true Allan variance, <strong>and</strong> one would expect it to havea tighter confidence interval than in the previous example. This could beexpressed with the aid <strong>of</strong> the chi-squared distribution with two degrees <strong>of</strong>freedom.However, there is another option. One could also consider the sampleAllan variance obtained from the second <strong>and</strong> third frequency measurements,that is, the middle sample variance. This last sample Allan variance is notindependent <strong>of</strong>the other two, since it is made up <strong>of</strong>parts <strong>of</strong>each <strong>of</strong>the others.But this does not mean that it cannot be used to improve the estimate <strong>of</strong> thetrue Allan variance. It does mean that the new average <strong>of</strong> three sample Allanvariances is not distributed as chi squared with three degrees <strong>of</strong>freedom. The~i~IIIIII II, I. I, I. I.TIMEYz. Yl' <strong>and</strong> Y. from five phaseFIG.12·12 Calculation <strong>of</strong> four frequency values ji"Feasurements at limes C, • C,. Cl. I•• <strong>and</strong> Is. The sample variance formed from YI <strong>and</strong> Y2 <strong>and</strong> theone formed from Y3 <strong>and</strong> j. are independent. The sample variance fonned from Y2 <strong>and</strong> YJ is nolindependent <strong>of</strong> the other two but does contain some additional information useful in estimating~he true sample variance.IN-81

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