diff --git a/Manuscript/FarDFT.tex b/Manuscript/FarDFT.tex
index 5dfcaa9..82d1c2f 100644
--- a/Manuscript/FarDFT.tex
+++ b/Manuscript/FarDFT.tex
@@ -71,7 +71,7 @@
 \newcommand{\VWN}{\text{VWN5}}
 \newcommand{\SVWN}{\text{SVWN5}}
 \newcommand{\LIM}{\text{LIM}}
-\newcommand{\CID}{\text{CID}}
+\newcommand{\MOM}{\text{MOM}}
 \newcommand{\Hxc}{\text{Hxc}}
 \newcommand{\Ha}{\text{H}}
 \newcommand{\ex}{\text{x}}
@@ -584,9 +584,9 @@ Equation \eqref{eq:becw} can be recast
 \label{eq:eLDA}
 \begin{split}
 	\be{\co}{\ew{}}(\n{}{}) 
-	& =  \e{\co}{\LDA}(\n{}{}) + \ew{} \qty[\e{\co}{(1)}(\n{}{}) - \e{\co}{(0)}(\n{}{})]
+	& =  \e{\co}{\VWN}(\n{}{}) + \ew{} \qty[\e{\co}{(1)}(\n{}{}) - \e{\co}{(0)}(\n{}{})]
 	\\
-	& =  \e{\co}{\LDA}(\n{}{}) + \ew{} \pdv{\e{\co}{\ew{}}(\n{}{})}{\ew{}},
+	& =  \e{\co}{\VWN}(\n{}{}) + \ew{} \pdv{\e{\co}{\ew{}}(\n{}{})}{\ew{}},
 \end{split}
 \end{equation}
 which nicely highlights the centrality of the LDA in the present weight-dependent density-functional approximation for ensembles.
@@ -620,9 +620,14 @@ For comparison purposes, we also report the linear interpolation method (LIM) ex
 \begin{equation}
 	\Ex{\LIM}{(1)} = 2 (\E{}{\ew{}=1/2} - \E{}{\ew{}=0}),
 \end{equation}
-as well as the MOM excitation energies.
-We point out that the MOM excitation energy is obtained by the difference in energy between the doubly-excited state at $\ew{} = 1$ and the ground-state at $\ew{} = 0$.
-MOM excitation energies can then be obtained via GOK-DFT ensemble calculations by performing a linear interpolation between $\ew{} = 0$ and $\ew{} = 1$.
+as well as the MOM excitation energies. \cite{Gilbert_2008,Barca_2018a,Barca_2018b}
+We point out that the MOM excitation energy is obtained by the difference in energy between the doubly-excited state at $\ew{} = 1$ and the ground state at $\ew{} = 0$.
+MOM excitation energies can then be obtained via GOK-DFT ensemble calculations by performing a linear interpolation between $\ew{} = 0$ and $\ew{} = 1$, \ie,
+\begin{equation}
+	\Ex{\MOM}{(1)} = \E{}{\ew{}=1} - \E{}{\ew{}=0}.
+\end{equation}
+
+The results gathered in Table \ref{tab:BigTab_H2} show that the GOK-DFT excitation energies obtained with the GIC-SeVWN5 functional at zero weight are the most accurate with an improvment of $0.25$ eV as compared to GIC-SVWN5
 
 %%% TABLE I %%%
 \begin{table*}