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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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Proc. 35th Ann. Freq. Control Symposium, USAERADC0I1, Ft. ~Ionmouth, UJ 07703, May 1981A MODIFIED "ALLAN VARIANCE" WITH INCREASEDOSCILLATOR CHARACTERIZATION ABILITYDavid W.Allan <strong>and</strong> James A. BarnesTime <strong>and</strong> Frequency DivisionNational Bureau <strong>of</strong> St<strong>and</strong>ardsBoulder, Colorado 80303Summarythe same, Le., - t-2. It is not at all uncommonHer~t<strong>of</strong>ore, the "Allan Variance," cr 2(t), hasbecome the de facto st<strong>and</strong>ard for measuring oscillatorinstabil ity in the time-domain. Often osci 11 ators for t <strong>of</strong> the order <strong>of</strong> one second <strong>and</strong>for white PM <strong>and</strong> flick.er PM to occur in precisionoscill ator frequency instabil iti es are resonabJ,ymodel able with a power law spectrum: Sshorter. The modified Allan variance, as developedin this paper, depends as t- 2 for or ::: +1 <strong>and</strong> as(f) ~ ,...,where y is the normal i zed frequency. y f is theFourier frequency, <strong>and</strong> or is a constant over somet-range <strong>of</strong> Fourier frequencies. It has been shown3 for or ::: +2. This yields a clear distinction inthat for power law spectrum cr 2(t) ~ t~, <strong>and</strong> that the time domain between these heret<strong>of</strong>ore somewhat~ ::: -or-1 for -3

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