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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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230 SAMUEL R. STEINThe combination <strong>of</strong> oscillator, frequency synthesizer, <strong>and</strong> mixer functions asa divider <strong>and</strong> scaler I functions as the system clock, recording elapsed time inunits <strong>of</strong> cycles <strong>of</strong> oscillator 1.The signals from oscillators 1 <strong>and</strong> 2 are represented according to Eq.(12-52) with 4>J 0 = 4>20 = 0, <strong>and</strong> the signal from the synthesizer is writtenv,,(t) = v"o cos[2XVs<strong>of</strong> + 4>.(r)]. (12-85)The phase <strong>of</strong> the synthesizer retards nearly linearly in time compared to thephase <strong>of</strong> oscillators 1 <strong>and</strong> 2. At time t..., the synthesizer reaches phasequadrature with oscillator I <strong>and</strong> the beat signal crosses zero (in the positivedirection), producing a pulse from the zero-crossing detector <strong>and</strong> startingthe time-interval counter. At a later time t N the continued sweep <strong>of</strong> thesynthesizer has brought it into quadrature with oscillator 2, <strong>and</strong> a pulse isproduced that stops the time-interval counter. The phase difference betweenthe oscillators can be written in terms <strong>of</strong> the three counter readings:(12-86)where N is the reading <strong>of</strong> scaler 2, M the reading <strong>of</strong> scaler 1, P the reading <strong>of</strong>the time-interval counter, <strong>and</strong> '0 the period <strong>of</strong> its time base (Stein er aI., 1983).Comparison with Eq. (12-45) for direct time-interval measurements revealsthat the role <strong>of</strong> the scalers is to accumulate the coarse phase differencebetween the oscillators, while the time-interval counter provides fine-grainresolution <strong>of</strong> the fractional cycle. This process is illustrated in Fig. 12-28. Theadvantage <strong>of</strong> the technique over direct time-interval measurements is that thenoise performance is improved by the large heterodyne factor, allowing timeresolution <strong>of</strong> 0.1 psec to be obtained. The synthesizer degrades the noiseperformance very little since it contributes to the noise only over the interval'eP'_______ .1:--- -o:~""bJI 000III0000000TIMEFIG.12-28 Total elapsed phase measured b} the dual-mixer system <strong>of</strong> Fig. 11-17 (solidlinel. This phase mea~urement consists <strong>of</strong> two components: the number <strong>of</strong> full cycles that haveelapsed is [he step function ploned as a dashed line: the fractional cycle is the saw-tooth functionploned as open circles.TN-lOO

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