Maréchal approximation
= Maréchal approximation
{c}
{title2=$S\simeq e^{-\sigma_\phi^2}$}
For small residual phase errors, $S\simeq e^{-\sigma_\phi^2}$, where $\sigma_\phi=2\pi h_{\rm rms}/\lambda$. The variance is taken after removing irrelevant constant phase. This approximation to the <Strehl ratio> is most useful near the <diffraction limit of a telescope>.