deletions | additions       diff --git a/Concepts_3.tex b/Concepts_3.tex  index 4df5e35..a9cca5e 100644  --- a/Concepts_3.tex  +++ b/Concepts_3.tex 
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due to different quantum yields of donor and acceptor dyes and/or  different photon detection efficiencies of donor and acceptor channels.  An alternative method to apply the $\gamma$ correction is to randomly  discard a fixed constant  fraction of photons chosen randomly  from either the DexDem or DexAem photon stream as proposed by~\cite{tsukanov_detailed_2013}. stream~\cite{Nir_2006}.  This simple and elegant method transforms the measurement data in order to  achieve $\gamma=1$, overcoming issues the issue  of selection bias between populations. This approach has also the advantage of preserving  the binomial distribution of D and A photons in each burst, so that peaks  of FRET populations are easier to model statistically.  The only drawbackof this method  is that, by discarding a fraction of photons, it this method  leads to information loss and therefore to potentially decreased a potential   decrease in  sensitivity and/or accuracy. A simple way to mitigate the dependence of the FRET distribution on   diff --git a/FRETBursts authorea latex/full_article.tex b/FRETBursts authorea latex/full_article.tex  index e54fe11..9219ce0 100644  --- a/FRETBursts authorea latex/full_article.tex  +++ b/FRETBursts authorea latex/full_article.tex 
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due to different quantum yields of donor and acceptor dyes and/or  different photon detection efficiencies of donor and acceptor channels.  An alternative method to apply the $\gamma$ correction is to randomly  discard a fixed constant  fraction of photons chosen randomly  from either the DexDem or DexAem photon stream as proposed by~\cite{tsukanov_detailed_2013}. stream~\cite{Nir_2006}.  This simple and elegant method transforms the measurement data in order to  achieve $\gamma=1$, overcoming issues the issue  of selection bias between populations. This approach has also the advantage of preserving  the binomial distribution of D and A photons in each burst, so that peaks  of FRET populations are easier to model statistically.  The only drawbackof this method  is that, by discarding a fraction of photons, it this method  leads to information loss and therefore to potentially decreased a potential   decrease in  sensitivity and/or accuracy. A simple way to mitigate the dependence of the FRET distribution on  the burst size selection threshold is weighting bursts proportionally to their size