An ideal oscillator provides a signal of constant frequency ν0 and amplitude V0: V(t) = V0 cos (2πν0t).
In practice, noise sources internal to the oscillator circuit induce random modulation of the signal's phase and amplitude. The real signal is then represented by :V(t) = V0[1 + α(t)] cos [2πν0t + ϕ(t)]
where ϕ(t) and α(t) are random variables representing phase modulation and amplitude modulation of the signal by noise, respectively. We then define the power spectral densities Sϕ(f ) and Sα(f ), which characterize the frequency distribution of ϕ(t) and α(t). In the case of an oscillator, the saturation...
You do not have access to this resource.
Exclusive to subscribers. 97% yet to be discovered!
(1) - RUTMAN (J.) - Characterization of Phase and Frequency Instabilities in Precision Frequency Sources : 15 years of Progress (Caractérisation des instabilités de phase et de fréquence : 15 ans de progrès) - . Proceedings of IEEE, 66, 9, 1048-1075 (sept. 1978).
(2) - CHRONOS - La mesure...
You do not have access to this resource.
Exclusive to subscribers. 97% yet to be discovered!
This offer includes interactive articles. Their quizzes highlight the key information to remember and validate their acquisition: from reader to player, you can enrich your knowledge.
You can easily identify them thanks to this pictogram: