saving work

Manuscript/FarDFT.tex

@@ -364,7 +364,7 @@ makes the ensemble much more linear (see Fig.~\ref{fig:Ew_H2}), and the excitati
 As readily seen from Eq.~\eqref{eq:Cxw}, $\Cx{\ew{}}$ reduces to $\Cx{}$ for $\ew{} = 0$.
 Note that we are not only using data from $\ew{} = 0$ to $\ew{} = 1/2$, but we also consider $1/2 < \ew{} \le 1$.
 We ensure that the weight-dependent functional does not affect the two ghost-interaction-free limit at $\ew{} = 0$ and $1$.
- 
+It is interesting to note that, around $\ew{} = 0$, the behavior of Eq.~\eqref{eq:Cxw} is linear 
 \begin{figure}
 	\includegraphics[width=0.8\linewidth]{Cx_H2}
 	\caption{
@@ -373,7 +373,7 @@ We ensure that the weight-dependent functional does not affect the two ghost-int
 	}
 \end{figure}
 
-In a third time, we add up correlation via the VWN5 local correlation functional. \cite{Vosko_1980}
+Third, we add up correlation via the VWN5 local correlation functional. \cite{Vosko_1980}
 For the sake of clarity, the explicit expression of the VWN5 functional is not reported here but it can be found in Ref.~\onlinecite{Vosko_1980}.
 The combination of the Slater and VWN5 functionals (SVWN5) yield a highly non-linear ensemble energy (as shown in Fig.~\ref{fig:Ew_H2}), while the combination of the MSFL and VWN5 functionals exhibit a small curvature and improved excitation energies, especially at small weights.
 
@@ -608,14 +608,14 @@ $\pdv{\E{\xc}{(1-\xi,\xi)}[\n{}{}]}{\xi}$ dans l'intégrale, non ? Can it be :
 %%% TABLE I %%%
 \begin{table*}
 \caption{
-Excitation energies (in eV) of \ce{H2} with $\RHH = 1.4$ bohr for various methods and basis sets.
+Excitation energies (in eV) associated with the lowest double excitation of \ce{H2} with $\RHH = 1.4$ bohr for various methods and basis sets.
 \label{tab:Energies}
 }
 \begin{ruledtabular}
 \begin{tabular}{llccccc}
-	\mc{2}{c}{xc functional} 	\\
+	\mc{2}{c}{xc functional} 		&					&	\mc{2}{c}{GOK}	\\
-	\cline{1-2}
+	\cline{1-2}												\cline{4-5}
-	exchange	&	correlation		&	Basis			&	GOK($\ew{} = 0$)	&	GOK($\ew{} = 1/2$)	&	LIM		&	MOM		\\
+	exchange	&	correlation		&	Basis			&	 $\ew{} = 0$	&	$\ew{} = 1/2$	&	LIM		&	MOM		\\
 	\hline
 	HF			&					&	aug-cc-pVDZ		&	38.52			&	30.86			&	34.55	&	28.65	\\
 				&					&	aug-cc-pVTZ		&	38.58			&	35.82			&	35.68	&	28.65	\\