deletions | additions       diff --git a/no_non_radiative_recombination_processes__.md b/no_non_radiative_recombination_processes__.md  index de786ab..f013783 100644  --- a/no_non_radiative_recombination_processes__.md  +++ b/no_non_radiative_recombination_processes__.md 
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no **no  non-radiative recombination processes : :**  The SQ limit only assumes radiative recombination as the only recombination channel for the cell, which is not the case in real materials. The magnitude of these non-radiative recombination losses can be characterized by the internal fluorescence efficiency, via the formula:  \[ \nu_{int\;fluo} = \frac{R_{rad}}{R_{rad}+R_{non-rad}} \]  To maximize \(\nu_{int\;fluo}\) we have to minimize \(R_{non-rad}\), which means optimizing the carrier lifetime for the recombination process. This can be modelled via 3 processes: the Shockley-Read-Hall (SRH), band to band, and Auger.