diff --git a/gating_table.tex b/gating_table.tex
index ce90b5f..ef64049 100644
--- a/gating_table.tex
+++ b/gating_table.tex
@@ -21,6 +21,7 @@ RS pyramidal,		        & \(\textrm{I}_{\textrm{Na}}\) inactivation
     
 
     \end{tabular}}
-      \caption[Gating Properties]{ For comparability to typical electrophysiological data fitting reported and for ease of further gating curve manipulations, a Boltzmann \(x_\infty = {\left(\frac{1-a}{1+{exp[{\frac{V-V_{1/2}}{k}}]}} +a\right)^j}\) 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 \cite{pospischil_minimal_2008} models where \(\alpha_x\) and \(\beta_x\) are used. Gating parameters for  \(\textrm{I}_{\textrm{K}_{\textrm{V}}\textrm{1.1}}\ \) are taken from \cite{ranjan_kinetic_2019} and fit to mean wild type parameters in \cite{lauxmann_therapeutic_2021}. Model gating not listed are taken directly from source publication.}
+      \caption[Gating Properties]{ For comparability to typical electrophysiological data fitting reported and for ease of further gating curve manipulations, a sigmoid function (eqn.\ref{eqn:Boltz}) %Boltzmann \(x_\infty = {\left(\frac{1-a}{1+{exp[{\frac{V-V_{1/2}}{k}}]}} +a\right)^j}\) 
+       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 \citet{pospischil_minimal_2008} models where \(\alpha_x\) and \(\beta_x\) are used. Gating parameters for  \(\textrm{I}_{\textrm{K}_{\textrm{V}}\textrm{1.1}}\ \) are taken from \citet{ranjan_kinetic_2019} and fit to mean wild type parameters in \citet{lauxmann_therapeutic_2021}. Model gating not listed are taken directly from source publication.}
     \label{tab:gating}
 \end{table}
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