diff --git a/manuscript.tex b/manuscript.tex
index ac037be..706bcfc 100644
--- a/manuscript.tex
+++ b/manuscript.tex
@@ -226,7 +226,7 @@ All modelling and simulation was done in parallel with custom written Python 3.8
     \begin{equation}\label{eqn:Boltz}
          x_\infty = {\left(\frac{1-a}{1+{\exp\left[{\frac{V-V_{1/2}}{k}}\right]}} +a\right)^j} 
     \end{equation}
-with slope \(k\), voltage for half-maximal activation or inactivation (\(V_{1/2}\)), exponent \(j\), and persistent current \(0 \leq a \leq 1\) were fitted for the RS pyramidal, RS inhibitory and FS models \cite{pospischil_minimal_2008} \notels{this reference could be missleading, they didnt't fit these parameters and the model origin is cited above} \notenk{how about ``... were fitted to the original formulism for RS pyramidal, RS inhibitory and FS models from \citet{pospischil_minimal_2008}.''}.  The properties of \IKv  were fitted to the mean wild type biophysical parameters of \Kv \citep{lauxmann_therapeutic_2021}.
+with slope \(k\), voltage for half-maximal activation or inactivation (\(V_{1/2}\)), exponent \(j\), and persistent current \(0 \leq a \leq 1\) were fitted to the original formulism for RS pyramidal, RS inhibitory and FS models from \citet{pospischil_minimal_2008}. The properties of \IKv  were fitted to the mean wild type biophysical parameters of \Kv \citep{lauxmann_therapeutic_2021}.
 
     
 \input{g_table}