What is the rms period jitter of the sinusoid in additive white noise from Example 19.9?
Again assuming the noise is much smaller than the amplitude of oscillation, \sigma _{n} ~«~ A , it was shown in Example 19.9 that the absolute jitter is also white. Hence, the phase noise is constant. Combining (19.57)
\sigma ^{2}_{\tau } = \frac{\sigma ^{2}_{n}}{A^{2} \omega _{0}^{2}} (19.57)
and (19.60)
\sigma ^{2}_{\tau } = \left\lgroup\frac{T_{0}}{2\pi } \right\rgroup ^{2} \int\limits_{0}^{1/2T_{0}}{S_{\phi }(f)df} (19.60)
therefore yields
S_{\phi }(f) =\left\lgroup\frac{8\pi ^{2}}{T_{0}} \right\rgroup \left\lgroup\frac{\sigma _{n}^{2}}{A^{2}\omega _{0}^{2}} \right\rgroup = \frac{2T_{0}\sigma _{n}^{2}}{A^{2}} (19.69)
Integration in (19.64)
\sigma ^{2}_{J} = \left\lgroup\frac{T_{0}}{\pi } \right\rgroup ^{2} \int\limits_{0}^{1/2T_{0}}{\sin ^{2}(\pi fT_{0})S_{\phi }(f)df} (19.64)
gives the variance of the period jitter.
\sigma ^{2}_{J} = \frac{2\sigma _{n}^{2}}{A^{2}\omega _{0}^{2}} (19.70)
The rms period jitter is the square root of (19.70).