diff --git a/Manuscript/srDFT_SC.tex b/Manuscript/srDFT_SC.tex
index 9cc8515..9c7ba4c 100644
--- a/Manuscript/srDFT_SC.tex
+++ b/Manuscript/srDFT_SC.tex
@@ -281,9 +281,6 @@
 \author{Emmanuel Giner}
 \email{emmanuel.giner@lct.jussieu.fr}
 \affiliation{\LCT}
-\author{Barth\'el\'emy Pradines}
-\affiliation{\LCT}
-\affiliation{\ISCD}
 \author{Anthony Scemama}
 \affiliation{\LCPQ}
 \author{Pierre-Fran\c{c}ois Loos}
@@ -603,11 +600,6 @@ We then define three complementary functionals:
 	\label{eq:def_pbeueg_ii}
 	\bar{E}^\Bas_{\pbeontXi} =  \int  \d\br{} \,\denr  \ecmd(\argrpbeontXi),  
 \end{equation}
-%\item[iii)] $\pbeuegns$ which combines a zero spin polarization and the UEG on-top pair density of Eq.~\eqref{eq:def_n2ueg}:
-%\begin{equation}
-%	\label{eq:def_pbeueg_iii}
-%	\bar{E}^\Bas_{\pbeuegns}  =  \int  \d\br{} \,\denr  \ecmd(\argrpbeuegns),
-%\end{equation}
 \item[iii)] $\pbeontns$ which combines a zero spin polarization and the on-top pair density of Eq.~\eqref{eq:def_n2extrap}:
 \begin{equation}
 	\label{eq:def_pbeueg_iv}
@@ -652,16 +644,8 @@ The performance of each of these functionals is tested in the following. Note th
 \ce{H10} & cc-pVDZ           &  622.1 [43.3]            &   642.6 [22.8]         &   649.2  [16.2]          &     649.5  [15.9]           \\
          & cc-pVTZ           &  655.2 [10.2]            &   661.9 [3.5]          &   666.0  [-0.6]          &     666.0  [-0.6]           \\
          & cc-pVQZ           &  661.2 [4.2]             &   664.1 [1.3]          &   666.4  [-1.0]          &     666.5  [-1.1]           \\[0.1cm]
-%\cline{2-6}
   	&	&\multicolumn{4}{c}{Estimated exact:\fnm[1] 665.4} \\[0.2cm]
 \hline
-%    		&         		& \tabc{exFCI}                    &   \tabc{exFCI+$\pbeuegXi$}   &   \tabc{exFCI+$\pbeontXi$}   &     \tabc{exFCI+$\pbeontns$}\\
-%\hline
-%\ce{C2} &  aug-cc-pVDZ          &   204.6  [29.5]         &   218.0  [16.1]     &   217.4  [16.7]     &     217.0  [17.1]           \\
-%      & aug-cc-pVTZ          &   223.4  [10.9]         &   228.1  [6.0]      &   228.6  [5.5]      &     226.5  [5.6]            \\[0.1cm]
-%\cline{2-6}
-% 	&	 & \multicolumn{4}{c}{Estimated exact:\fnm[2] 234.1} \\[0.2cm]
-%\hline                                                                                                                 
     		&         		& \tabc{exFCI}                    &   \tabc{exFCI+$\pbeuegXi$}   &   \tabc{exFCI+$\pbeontXi$}   &     \tabc{exFCI+$\pbeontns$}\\
 \hline                                                                                                                 
 \ce{N2} & aug-cc-pVDZ          &   321.9  [40.8]         &   356.2  [6.5]           &   355.5  [7.2]           &     354.6  [8.1]           \\
@@ -745,18 +729,6 @@ Analyzing more carefully the performance of the different types of approximate f
 
 
 
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-%\begin{figure*}
-%        \includegraphics[width=0.45\linewidth]{data/C2/DFT_avdzE_relat.pdf}
-%        \includegraphics[width=0.45\linewidth]{data/C2/DFT_avdzE_relat_zoom.pdf}
-%        \includegraphics[width=0.45\linewidth]{data/C2/DFT_avtzE_relat.pdf}
-%        \includegraphics[width=0.45\linewidth]{data/C2/DFT_avtzE_relat_zoom.pdf}
-%        \caption{
-%        Potential energy curves of the \ce{C2} molecule calculated with exFCI and basis-set corrected exFCI using the aug-cc-pVDZ (top) and aug-cc-pVTZ (bottom) basis sets. The estimated exact energies are based on fit of experimental data and obtained from Ref.~\onlinecite{LieCle-JCP-74a}.
-%        \label{fig:C2}}
-%\end{figure*}
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-
 
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \begin{figure*}
@@ -775,21 +747,8 @@ The estimated exact energies are based on a fit of experimental data and obtaine
 \end{figure*}
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-%\begin{figure*}
-%        \includegraphics[width=0.45\linewidth]{data/F2/DFT_vdzE_relat.pdf}
-%        \includegraphics[width=0.45\linewidth]{data/F2/DFT_vdzE_relat_zoom.pdf}
-%        \includegraphics[width=0.45\linewidth]{data/F2/DFT_vtzE_relat.pdf}
-%        \includegraphics[width=0.45\linewidth]{data/F2/DFT_vtzE_relat_zoom.pdf}
-%        \includegraphics[width=0.45\linewidth]{data/F2/DFT_vqzE_relat.pdf}
-%        \includegraphics[width=0.45\linewidth]{data/F2/DFT_vqzE_relat_zoom.pdf}
-%        \caption{
-%        Potential energy curves of the \ce{F2} molecule calculated with CEEIS$^1$ and basis-set corrected CEEIS$^1$ using the cc-pVDZ (top), cc-pVTZ (middle) and cc-pVQZ (bottom) basis sets. 
-%        The estimated exact energies are based on a fit of the valence-only extrapolated CEEIS data extracted from Ref.~\onlinecite{BytNagGorRue-JCP-07}.
-%        \label{fig:F2}}
-%\end{figure*}
-%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \begin{figure*}
  	\subfigure[aug-cc-pVDZ]{
         \includegraphics[width=0.45\linewidth]{data/F2/DFT_avdzE_relat.pdf}