diff --git a/Manuscript/H2_BSE.pdf b/Manuscript/H2_BSE.pdf
index 25fa5b7..064cdd1 100644
Binary files a/Manuscript/H2_BSE.pdf and b/Manuscript/H2_BSE.pdf differ
diff --git a/Manuscript/sfBSE.tex b/Manuscript/sfBSE.tex
index 6a70dfb..58d91a2 100644
--- a/Manuscript/sfBSE.tex
+++ b/Manuscript/sfBSE.tex
@@ -819,15 +819,15 @@ Now, looking at the Table~\ref{tab:CBD_D4h} and comparing SF-BSE@{\GOWO} to SF-A
 			Method					&	$1\,{}^3B_{1g}$	&	$1\,{}^1B_{1g}$	&	$2\,{}^1A_{1g}$	\\
 			\hline
 			SF-TD-BLYP \fnm[3] & & & \\
-			SF-TD-B3LYP \fnm[3] & & & \\
+			SF-TD-B3LYP \fnm[3] &1.750 &2.260 &4.094 \\
 			SF-TD-BH\&HLYP\fnm[3] &1.583 &2.813 & 4.528\\
 			SF-CIS\fnm[1]			&	&	&	\\
 			EOM-SF-CCSD\fnm[1]			&1.654	&	3.416&4.360	\\
 			EOM-SF-CCSD(fT)\fnm[1]		&	1.516&	3.260&4.205	\\
 			EOM-SF-CCSD(dT)\fnm[1]		&1.475	&3.215	&4.176	\\
-			SF-ADC(2)-s\fnm[2]			&	1.572&	3.201&	4.241\\
-			SF-ADC(2)-x\fnm[2]			&1.576	&3.134	&3.792	\\
-			SF-ADC(3)\fnm[2]			&	1.455&3.276	&4.328	\\
+			SF-ADC(2)-s\fnm[2]			&	1.573&	3.208&	4.247\\
+			SF-ADC(2)-x\fnm[2]			&1.576	&3.141	&3.796	\\
+			SF-ADC(3)\fnm[2]			&	1.456&3.285	&4.334	\\
 			SF-BSE@{\GOWO}\fnm[3] 		& 1.438	& 2.704	&4.540 	\\
 			SF-dBSE@{\GOWO}\fnm[3]		& 1.403	&2.883	&4.621	\\
 		\end{tabular}
@@ -851,13 +851,13 @@ Now, looking at the Table~\ref{tab:CBD_D4h} and comparing SF-BSE@{\GOWO} to SF-A
 			Method					&	$1\,{}^3A_{2g}$	&	$2\,{}^1A_{1g}$	&	$1\,{}^1B_{2g}$	\\
 			\hline
 			SF-TD-BLYP \fnm[3] & & & \\
-			SF-TD-B3LYP \fnm[3] & & & \\
-			SF-TD-BH\&HLYP\fnm[3] & & & \\
+			SF-TD-B3LYP \fnm[3] &-0.020 & 0.486& 0.547\\
+			SF-TD-BH\&HLYP\fnm[3] &0.048 & 1.282&1.465 \\
 			SF-CIS\fnm[1]			&0.317	&	3.125&2.650	\\
 			EOM-SF-CCSD\fnm[1]			&0.369	&	1.824&	2.143\\
 			EOM-SF-CCSD(fT)\fnm[1]		&	0.163&1.530	&1.921	\\
 			EOM-SF-CCSD(dT)\fnm[1]		&0.098	&1.456	&1.853	\\
-			SF-ADC(2)-s\fnm[2]			& 0.265	&	1.658& 1.904	\\
+			SF-ADC(2)-s\fnm[2]			& 0.266&	1.664& 1.910	\\
 			SF-ADC(2)-x\fnm[2]			&	0.217&1.123	&1.799	\\
 			SF-ADC(3)\fnm[2]			&0.083	&1.621	&1.930	\\
 			SF-BSE@{\GOWO}\fnm[3] 		& -0.049	& 1.189	& 1.480	\\