From a05227b9991067661f74da767761fcce743470f3 Mon Sep 17 00:00:00 2001
From: Pierre-Francois Loos <pierrefrancois.loos@gmail.com>
Date: Wed, 8 Apr 2020 14:14:01 +0200
Subject: [PATCH] H2 res

---
 Manuscript/FarDFT.bib | 12 +++++++++++-
 Manuscript/FarDFT.tex |  3 ++-
 2 files changed, 13 insertions(+), 2 deletions(-)

diff --git a/Manuscript/FarDFT.bib b/Manuscript/FarDFT.bib
index a96da14..8683b38 100644
--- a/Manuscript/FarDFT.bib
+++ b/Manuscript/FarDFT.bib
@@ -1,13 +1,23 @@
 %% This BibTeX bibliography file was created using BibDesk.
 %% http://bibdesk.sourceforge.net/
 
-%% Created for Pierre-Francois Loos at 2020-04-08 13:05:55 +0200 
+%% Created for Pierre-Francois Loos at 2020-04-08 14:13:22 +0200 
 
 
 %% Saved with string encoding Unicode (UTF-8) 
 
 
 
+@article{Fromager_2020,
+	Archiveprefix = {arXiv},
+	Author = {Emmanuel Fromager},
+	Date-Added = {2020-04-08 14:13:18 +0200},
+	Date-Modified = {2020-04-08 14:13:18 +0200},
+	Eprint = {2001.08605},
+	Primaryclass = {physics.chem-ph},
+	Title = {Individual correlations in ensemble density-functional theory: State-driven/density-driven decomposition without additional Kohn-Sham systems},
+	Year = {2020}}
+
 @article{Bottcher_1974,
 	Author = {C. Bottcher and K. Docken},
 	Date-Added = {2020-04-08 13:03:40 +0200},
diff --git a/Manuscript/FarDFT.tex b/Manuscript/FarDFT.tex
index 82d1c2f..28c4178 100644
--- a/Manuscript/FarDFT.tex
+++ b/Manuscript/FarDFT.tex
@@ -627,7 +627,8 @@ MOM excitation energies can then be obtained via GOK-DFT ensemble calculations b
 	\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
+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 improvement of $0.25$ eV as compared to GIC-SVWN5, which is due to the ensemble derivative contribution of the eVWN5 functional.
+The GIC-SeVWN5 excitation energies at equi-weights (\ie, $\ew{} = 1/2$) are less satisfactory, but still remains in good agreement with FCI, with again a small improvement as compared to GIC-SVWN5.
 
 %%% TABLE I %%%
 \begin{table*}