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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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t ....chi -square. d. f. is the number <strong>of</strong> degrees <strong>of</strong>AfL +.. "* .... freedom (possibly not an integer), <strong>and</strong> a 2 is the/f 4---~---4----~---~---"'t 1"""true" Allan Variance we're all interested ink- 1-I+- 2_1+- ~~ J<strong>of</strong> ~ knowing--but can only estimate imperfectly.I+- ~ BUR: -+I+-~~-+'Chi-square is a r<strong>and</strong>om variable <strong>and</strong> its distri­r----------, bution has been studied extensively. For some:14-~~~ : reason, chi-square is defined so that d. f., the... _--------_ ....number <strong>of</strong> degrees <strong>of</strong> freedom. appears explicitlyFIGURE 5.2 in eq (5.1). Still, X 2 is a (implicit)first pair <strong>and</strong> calculate a sample Allan Variance.function <strong>of</strong> d. f., also.<strong>and</strong> we could calculate a second sample Allan The probability density for the chi-squareVariance from the second pair (i.e.• the third <strong>and</strong>distribution is given by the relationfourth frequency measurements). The average <strong>of</strong>these two sample Allan Variances provides an d. f.-1 X1 2improved estimate <strong>of</strong> the "true" Allan Variance, p(x 2 ) = (x 2 T e (5.2)<strong>and</strong> ~ewould expect it to have a tighter confidenceinterval than in the previous example.This couldbution with TWO degrees <strong>of</strong> freedom.However, the re is another option. We cou1dalso consider the sample Allan Variance obtainedfrom the second <strong>and</strong> third frequency measurements.That is the middle sample variance.Now. however,Chi-square distributions are useful in deterwe'rein trouble because clearly this last sampleA11 an Vari ance is NOTtwo.independent <strong>of</strong> the otherIndeed, it is made up <strong>of</strong> parts <strong>of</strong> each <strong>of</strong>the other two.Thi s does NOT mean that we can'tuse it for improving our estimate <strong>of</strong> the "true"Allan Variance, but it does mean that wecan'tjust assume that the new average <strong>of</strong> three sampleAllan Variances is distributed as chi-square withcounter chi-square distributions with fractionaldegrees <strong>of</strong> freedom.And as one might expect. thenumber <strong>of</strong> degrees <strong>of</strong> freedom will depend upon theunderlying noise type, that is, white FM. flick.erFM, or whatever.Before going on with this, it is <strong>of</strong> value toreview somebution. Sample variances (like sample Allantion:2d. f. r(d/.)where r(d;/ ") is the gamma function, defined bybe expressed with the aid <strong>of</strong> the chi-square distritheintegralOIlt-l ·xr (t) = J0 X e dx (5.3)mining specified confidence intervals for variances<strong>and</strong> st<strong>and</strong>ard deviations. Here is an example.Suppose we hav~a sample variance S2 = 3.0 <strong>and</strong> weknow that this variance has 10 degrees <strong>of</strong> fre~dom.(Just how we can k.now the degrees <strong>of</strong> freedom wi 11be discussed shortly.) Suppose a1so that we wantto know a range around our sample value <strong>of</strong> S2 = 3.0which "probably" contains the true value, a 2 .three degrees <strong>of</strong> freedom. Indeed, we will endesiredconfidence is, say, 90%.TheThat is, 10% <strong>of</strong>the time the true value will actually fall outside<strong>of</strong> the stated bounds.to a 11 ocate S%The usual way to proceed isto the low end <strong>and</strong> 5% to the hi ghend for errors, leaving our 90% in the middle.This is arbitrary <strong>and</strong> a specific problem mightdictate a different allocation. We now resort toconcepts <strong>of</strong> the chi-square distritables<strong>of</strong> the chi-square distribution <strong>and</strong> findthat for 10 degrees <strong>of</strong> freedom the 5% <strong>and</strong> 95%Variances) are distributed according to the equapointscorrespond to:x2(.05) :: 3.94x2. = (d. f. ) . 52(5.1)at for d.f. = 10 (5.4)where 52 is the sample Allan Variance, x2. is X 2 (.95) =18.314TN-27

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