diff --git a/Data/H2_aug-cc-pvtz_RGIC_H.dat b/Data/H2_aug-cc-pvtz_RGIC_H.dat
new file mode 100644
index 0000000..6d9479b
--- /dev/null
+++ b/Data/H2_aug-cc-pvtz_RGIC_H.dat
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diff --git a/Data/H2_aug-cc-pvtz_RGIC_RMFL20.dat b/Data/H2_aug-cc-pvtz_RGIC_RMFL20.dat
new file mode 100644
index 0000000..228c096
--- /dev/null
+++ b/Data/H2_aug-cc-pvtz_RGIC_RMFL20.dat
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diff --git a/Data/H2_aug-cc-pvtz_RGIC_RVWN5.dat b/Data/H2_aug-cc-pvtz_RGIC_RVWN5.dat
new file mode 100644
index 0000000..543d555
--- /dev/null
+++ b/Data/H2_aug-cc-pvtz_RGIC_RVWN5.dat
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diff --git a/Data/H2_aug-cc-pvtz_RS51_H.dat b/Data/H2_aug-cc-pvtz_RS51_H.dat
new file mode 100644
index 0000000..1cb29e8
--- /dev/null
+++ b/Data/H2_aug-cc-pvtz_RS51_H.dat
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diff --git a/Data/H2st_aug-cc-pvtz_RGIC_H.dat b/Data/H2st_aug-cc-pvtz_RGIC_H.dat
new file mode 100644
index 0000000..4c4e5cd
--- /dev/null
+++ b/Data/H2st_aug-cc-pvtz_RGIC_H.dat
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diff --git a/Data/H2st_aug-cc-pvtz_RS51_H.dat b/Data/H2st_aug-cc-pvtz_RS51_H.dat
new file mode 100644
index 0000000..c8fa03b
--- /dev/null
+++ b/Data/H2st_aug-cc-pvtz_RS51_H.dat
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diff --git a/Data/HNO_aug_cc-pvdz_RS51_H.dat b/Data/HNO_aug_cc-pvdz_RS51_H.dat
new file mode 100644
index 0000000..93500d3
--- /dev/null
+++ b/Data/HNO_aug_cc-pvdz_RS51_H.dat
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diff --git a/Data/He_aug-cc-pvtz_RGIC_H.dat b/Data/He_aug-cc-pvtz_RGIC_H.dat
new file mode 100644
index 0000000..a58f4f5
--- /dev/null
+++ b/Data/He_aug-cc-pvtz_RGIC_H.dat
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diff --git a/Data/He_aug-cc-pvtz_RGIC_RMFL20.dat b/Data/He_aug-cc-pvtz_RGIC_RMFL20.dat
new file mode 100644
index 0000000..d9c8012
--- /dev/null
+++ b/Data/He_aug-cc-pvtz_RGIC_RMFL20.dat
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diff --git a/Data/He_aug-cc-pvtz_RGIC_RVWN5.dat b/Data/He_aug-cc-pvtz_RGIC_RVWN5.dat
new file mode 100644
index 0000000..dd23a56
--- /dev/null
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diff --git a/Data/He_aug-cc-pvtz_RS51_H.dat b/Data/He_aug-cc-pvtz_RS51_H.dat
new file mode 100644
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--- /dev/null
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diff --git a/Data/He_d-aug-cc-pvqz_RS51_H.dat b/Data/He_d-aug-cc-pvqz_RS51_H.dat
new file mode 100644
index 0000000..8fe7e0c
--- /dev/null
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new file mode 100644
index 0000000..24a75b4
--- /dev/null
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diff --git a/Data/w/H2_aug-cc-pvtz_RCC_RMFL20.dat b/Data/w/H2_aug-cc-pvtz_RCC_RMFL20.dat
new file mode 100644
index 0000000..224d803
--- /dev/null
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new file mode 100644
index 0000000..c894ed1
--- /dev/null
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new file mode 100644
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diff --git a/Manuscript/Ew_H2.pdf b/Manuscript/Ew_H2.pdf
index dd50d67..e9a3b5f 100644
Binary files a/Manuscript/Ew_H2.pdf and b/Manuscript/Ew_H2.pdf differ
diff --git a/Manuscript/FarDFT.tex b/Manuscript/FarDFT.tex
index 338c52a..d0836fc 100644
--- a/Manuscript/FarDFT.tex
+++ b/Manuscript/FarDFT.tex
@@ -1045,6 +1045,9 @@ Nonetheless, it can be nicely described with a Gaussian basis set containing eno
 Consequently, we consider for this particular example the d-aug-cc-pVQZ basis set which contains two sets of diffuse functions.
 The excitation energies associated with this double excitation computed with various methods and combinations of xc functionals are gathered in Table \ref{tab:BigTab_He}.
 
+Before analysing the results, we would like to point out that, there is a large number of singly-excited states, between the $1s2s$ state and the $2s^2$.
+Therefore, the present ensemble is not consistent with GOK theory.
+
 The parameters of the CC-S weight-dependent exchange functional (computed with the smaller aug-cc-pVTZ basis) are $\alpha = +1.912\,574$, $\beta = +2.715\,267$, and $\gamma = +2.163\,422$ [see Eq.~\eqref{eq:Cxw}], the curvature of the ensemble energy being more pronounced in \ce{He} than in \ce{H2} (blue curve in Fig.~\ref{fig:Cxw}).
 The results reported in Table \ref{tab:BigTab_He} evidence this strong weight dependence of the excitation energies for HF or LDA exchange.
 
diff --git a/Manuscript/Om_H2.pdf b/Manuscript/Om_H2.pdf
index 8422b70..efb8a70 100644
Binary files a/Manuscript/Om_H2.pdf and b/Manuscript/Om_H2.pdf differ