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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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270 A. L. LANCE, W. D. SEAL, AND F. LABAARThe sensitivity (noise floor) <strong>of</strong> the two-oscillator measurement systemincludes the thermal <strong>and</strong> shot noise <strong>of</strong> the mixer <strong>and</strong> the noise <strong>of</strong> the baseb<strong>and</strong>preamplifier (referred to its input). This noise floor is measured withthe oscillator under test inoperative. The measurement system sensitivity <strong>of</strong>the two-oscillator system, on a per hertz density basis (dBc/Hz) iswhere bL: n is the rms noise voltage measured in a one-hertz b<strong>and</strong>width.The two-oscillator system therefore yields the output noise from bothoscillators. If the reference oscillator is superior in performance, as assumedin the previous discussions, then one obtains a direct measure <strong>of</strong> the noisecharacteristics <strong>of</strong> the oscillator under test. If the reference <strong>and</strong> test oscillatorsare the same type, a useful approximation is to assume that the measurednoise power is twice that associated with one noisy oscillator. This approximationis in error by no more than 3 dB for the noisier oscillator. Substitutingin Eq. (80) <strong>and</strong> using the relationships in Eq. (56), we have, per hertz,(83)!t'(f)1 = 2[(6V rm Y/(VPIP)2](2njr d )2 (84)dImExamination <strong>of</strong> this equation reveals the following.(I) The term in the brackets represents the two-oscillator response.<strong>Note</strong> that this term represents the noise floor oj the two-oscillator method.Therefore, adoption <strong>of</strong> the delay-line method results in a higher noise by thefactor (2rr.jr d )2 when compared with the two-oscillator measurement method.The sensitivity (noise floor) for delay lines with different values <strong>of</strong> time delayare illustrated in Fig. 17.(2) Equation (84) also indicates that the measured value <strong>of</strong> !t'(f) isperiodic in w = 2rrf This is shown in Fig. 21. The first null in the responsesis at the Fourier frequency j = l/rd' The periodicity indicates that the calibrationrange <strong>of</strong> the discriminator is limited <strong>and</strong> that valid measurementsoccur only in the indicated range. as verified by the discriminator slope shownin Fig. 16. (See Fig. 23.)(3) The maximum value <strong>of</strong> (2rrjr d )2 can be greater than unity (it is 4 atj = 1'2r d )· This 6-dB advantage is utilized in the noise-floor measurement.However, it is beyond the valid calibration range <strong>of</strong> the delay-line system.The 6-dB advantage is <strong>of</strong>fset by the line attenuation at microwave frequencies,as discussed by Halford (1975).The delay-line discriminator system has been analyzed in terms <strong>of</strong>a powerlimitedsystem (a particular idealized system in which the choice <strong>of</strong> poweroscillator voltage. the attenuator <strong>of</strong> the delay line, <strong>and</strong> the conversion lossTN-221

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