deletions | additions       diff --git a/Mode Visibility.tex b/Mode Visibility.tex  index 408d9ba..5352ed5 100644  --- a/Mode Visibility.tex  +++ b/Mode Visibility.tex 
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Modes suppressed via the magnetic greenhouse effect have an extra source of damping determined by the rate at which energy leaks through the evanescent region separating the acoustic cavity from the g-mode cavity. For suppressed modes, we assume that any mode energy which leaks into the g-mode cavity is completely lost via the magnetic greenhouse effect. Given some mode energy contained within the acoustic cavity, $E_{\rm ac}$, the rate at which mode energy leaks into the core is  \begin{equation}  \dot{E}_{\rm leak} = E_{\rm ac} \frac{T^2}{2 t_{\rm cross} cross}}  , \end{equation}  where $T$ is the transmission coefficient from equation \ref{eqn:integral}, and  \begin{equation}