TY - JOUR
T1 - Spectral Dispersion of Modulated Signals Due to Oscillator Phase Instability
T2 - White and Random Walk Phase Model
AU - Vannicola, Vincent C.
AU - Varshney, Pramod K.
PY - 1983/7
Y1 - 1983/7
N2 - This paper considers the modeling of oscillator phase instability and the resulting spectral dispersion. A phase covariance matrix method is developed for determining the autocorrelation function and the power spectral density of the oscillator sinusoidal RF signal when corrupted by a superposition of a white phase random process and a random walk phase random process. By limiting the discussion to phase covariance matrices, it is shown that the direct use of a certain class of nonstationary phase random processes leads to stationary RF signal autocorrelation functions and associated power spectral densities. This is so despite the nonstationary phase driving force. The procedures provided here are also applied towards the determination of the average autocorrelation function and the average spectrum when the cisoidal oscillator signal undergoes modulation. Modulating waveforms used as examples include the CW, the infinite pulse train, and the finite pulse train.
AB - This paper considers the modeling of oscillator phase instability and the resulting spectral dispersion. A phase covariance matrix method is developed for determining the autocorrelation function and the power spectral density of the oscillator sinusoidal RF signal when corrupted by a superposition of a white phase random process and a random walk phase random process. By limiting the discussion to phase covariance matrices, it is shown that the direct use of a certain class of nonstationary phase random processes leads to stationary RF signal autocorrelation functions and associated power spectral densities. This is so despite the nonstationary phase driving force. The procedures provided here are also applied towards the determination of the average autocorrelation function and the average spectrum when the cisoidal oscillator signal undergoes modulation. Modulating waveforms used as examples include the CW, the infinite pulse train, and the finite pulse train.
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U2 - 10.1109/TCOM.1983.1095902
DO - 10.1109/TCOM.1983.1095902
M3 - Article
AN - SCOPUS:0020781958
SN - 0090-6778
VL - 31
SP - 886
EP - 895
JO - IEEE Transactions on Communications
JF - IEEE Transactions on Communications
IS - 7
ER -