deletions | additions       diff --git a/subsection_Quadrature_Noise_The_motion__.tex b/subsection_Quadrature_Noise_The_motion__.tex  index 31c0d2b..eae7a68 100644  --- a/subsection_Quadrature_Noise_The_motion__.tex  +++ b/subsection_Quadrature_Noise_The_motion__.tex 
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\[ A_s \approx A_i\]  Also, we may write the frequencies in the form,  \[ \omega_{s, i} = \omega_p/2 \pm \delta \]  From the above eqs,it's easy to see that the signal is squeezed - the quadrature component is attenuated.  \[f(t) = A e^{i\omega_p/2 t}(e^{i \delta t} + e^{- i \delta t}) = 2A cos(\delta t) e^{i\omega_p/2 t} \]  The signal is squeezed - the quadrature component is attenuated and the in-phase component is amplified.