diff --git a/BSEdyn.tex b/BSEdyn.tex
index 7edfc08..887dde1 100644
--- a/BSEdyn.tex
+++ b/BSEdyn.tex
@@ -681,6 +681,7 @@ All the BSE calculations have been performed with our locally developed $GW$ sof
 	\caption{
 	Singlet excitation energies (in eV) for various molecules obtained with the aug-cc-pVTZ basis set at various levels of theory.
 	The dynamical correction is computed in the TDA.
+	CT and R stand respectively for charge transfer and Rydberg.
 	\label{tab:BigTabSi}
 	}
 	\begin{ruledtabular}
@@ -691,7 +692,7 @@ All the BSE calculations have been performed with our locally developed $GW$ sof
 									&	\tabc{$\Eg^{\GW}$}	&	\tabc{$\Om{m}{\stat}$}	&	\tabc{$\Om{m}{\dyn}$}	&	\tabc{$\Delta\Om{m}{\dyn}$}	&	\tabc{$Z_{m}$}		
 									&	\tabc{CIS(D)}	&	\tabc{ADC(2)}	&	\tabc{CCSD}	&	\tabc{CC2}	&	\tabc{CC3}	\\
 			\hline
-			\ce{HCl}	&	$^1\Pi$(CT)			&	13.43	&	8.30	&	8.19	&	-0.11	&	1.009	&	13.42	&	8.29	&	8.18	&	-0.11	&	1.010	&	6.07	&	7.97	&	7.91	&	7.96	&		7.84	\\
+			\ce{HCl}	&	$^1\Pi$(CT)			&	13.43	&	8.30	&	8.19	&	-0.11	&	1.009	&		&		&		&		&		&	6.07	&	7.97	&	7.91	&	7.96	&		7.84	\\
 			\\
 			\ce{H2O}	&	$^1B_1(n \ra 3s)$	&	13.58	&	8.09	&	8.00	&	-0.09	&	1.007	&		&	&	&	&	&	7.62	&	7.18	&	7.60	&	7.23	&	7.65	\\
 						&	$^1A_2(n \ra 3p)$	&			&	9.79	&	9.72	&	-0.07	&	1.005	&	&	&	&	&	&	9.41	&	8.84	&	9.36	&	8.89	&	9.43	\\
@@ -712,9 +713,12 @@ All the BSE calculations have been performed with our locally developed $GW$ sof
 						&	$^1\Sigma^+$(R)					&			&	12.39	&	12.37	&	-0.02	&	1.003	&	&	&	&	&	&	11.71	&	11.83	&	11.75	&	11.63	&	11.49	\\
 						&	$^1\Pi$(R)						&			&	12.37	&	12.32	&	-0.05	&	1.004	&	&	&	&	&	&	12.06	&	12.03	&	11.96	&	11.83	&	11.69	\\
 			\\
-			\ce{C2H4}	&	$^1B_{3u}(\pi \ra 3s)$		&	&	&	&	&	&	&	&	&	&	&	7.35	&	7.34	&	7.42	&	7.29	&	7.35	\\
-						&	$^1B_{1u}(\pi \ra \pis)$	&	&	&	&	&	&	&	&	&	&	&	7.95	&	7.91	&	8.02	&	7.92	&	7.91	\\
-						&	$^1B_{1g}(\pi \ra 3p)$		&	&	&	&	&	&	&	&	&	&	&	8.01	&	7.99	&	8.08	&	7.95	&	8.03	\\
+			\ce{HNO}	&	$^1A''(n \ra \pis)$				&	11.71	&	2.46	&	1.98	&	-0.48	&	1.035	&	&	&	&	&	&	1.80	&	1.68	&	1.76			&	1.74		&	1.75		\\
+						&	$^1A'$(R)						&			&	7.05	&	7.01	&	-0.037	&	1.003	&	&	&	&	&	&	5.81	&	5.73	&	6.30			&	5.72		&	6.26		\\
+			\\
+			\ce{C2H4}	&	$^1B_{3u}(\pi \ra 3s)$		&	11.49	&	7.64	&	&	&	&	&	&	&	&	&	7.35	&	7.34	&	7.42	&	7.29	&	7.35	\\
+						&	$^1B_{1u}(\pi \ra \pis)$	&			&	8.18	&	&	&	&	&	&	&	&	&	7.95	&	7.91	&	8.02	&	7.92	&	7.91	\\
+						&	$^1B_{1g}(\pi \ra 3p)$		&			&	8.29	&	&	&	&	&	&	&	&	&	8.01	&	7.99	&	8.08	&	7.95	&	8.03	\\
 			\\
 			\ce{CH2O}	&	$^1A_2(n \ra \pis)$		&	12.00	&	5.03	&	4.68	&	-0.35	&	1.027	&	&	&	&	&	&	4.04	&	3.92	&	4.01	&	4.07	&	3.97	\\
 						&	$^1B_2(n \ra 3s)$		&			&	7.87	&	7.85	&	-0.02	&	1.001	&		&	&	&	&	&	6.64	&	6.50	&	7.23	&	6.56	&	7.18	\\
@@ -757,9 +761,12 @@ All the BSE calculations have been performed with our locally developed $GW$ sof
 						&	$^3\Sigma_u^-(\pi \ra \pis)$	&			&	10.79	&	10.38	&	-0.42	&	1.034	&	&	&	&	&	&	10.10	&	10.01	&	9.81	&	10.27	&	9.82	\\
 						&	$^3\Sigma_u^+$(R)				&			&	11.48	&	11.38	&	-0.10	&	1.010	&	&	&	&	&	&	10.98	&	10.83	&	10.71	&	10.60	&	10.45	\\
 			\\
-			\ce{C2H4}	&	$^3B_{1u}(\pi \ra \pis)$	&	&	&	&	&	&	&	&	&	&	&	4.62	&	4.59	&	4.46	&	4.59	&	4.53	\\
-						&	$^3B_{3u}(\pi \ra 3s)$		&	&	&	&	&	&	&	&	&	&	&	7.26	&	7.23	&	7.29	&	7.19	&	7.24	\\
-						&	$^3B_{1g}(\pi \ra 3p)$		&	&	&	&	&	&	&	&	&	&	&	7.97	&	7.95	&	8.03	&	7.91	&	7.98	\\
+			\ce{HNO}	&	$^3A''(n \ra \pis)$				&	11.71	&	3.05	&	2.35		&	-0.71		&	1.069		&	&	&	&	&	&	0.91	&	0.78		&	0.85			&	0.84		&	0.88		\\
+						&	$^3A'(\pi \ra \pis)$			&			&	6.69	&	6.70		&	0.01		&	1.000		&	&	&	&	&	&	5.72	&	5.46		&	5.49			&	5.44		&	5.59		\\
+			\\
+			\ce{C2H4}	&	$^3B_{1u}(\pi \ra \pis)$	&	11.49	&	&	&	&	&	&	&	&	&	&	4.62	&	4.59	&	4.46	&	4.59	&	4.53	\\
+						&	$^3B_{3u}(\pi \ra 3s)$		&			&	&	&	&	&	&	&	&	&	&	7.26	&	7.23	&	7.29	&	7.19	&	7.24	\\
+						&	$^3B_{1g}(\pi \ra 3p)$		&			&	&	&	&	&	&	&	&	&	&	7.97	&	7.95	&	8.03	&	7.91	&	7.98	\\
 			\\
 			\ce{CH2O}	&	$^3A_2(n \ra \pis)$		&	12.00	&	5.53	&	5.05	&	-0.47	&	1.049	&	&	&	&	&	&	3.58	&	3.46	&	3.56	&	3.59	&	3.57	\\
 						&	$^3A_1(\pi \ra \pis)$	&			&	8.15	&	7.32	&	-0.83	&	1.067	&	&	&	&	&	&	6.27	&	6.20	&	5.97	&	6.30	&	6.05	\\
@@ -772,23 +779,23 @@ All the BSE calculations have been performed with our locally developed $GW$ sof
 \end{table*}
 
 %%% TABLE III %%%
-\begin{table}
-	\caption{
-	Excitation energies (in eV) of CN3 obtained with the aug-cc-pVDZ basis set  at various levels of theory.
-	%$\Eg^{\GW} = 13.79$ eV.		
-	\label{tab:CN3}
-	}
-	\begin{ruledtabular}
-		\begin{tabular}{lcc}
-							&	\mc{2}{c}{Excitation}	\\
-		Method				&	$^1B_2(\pi \ra \pis)$	&	$^3B_2(\pi \ra \pis)$		\\
-		\hline
-		BSE@{\GOWO}@HF			&	7.66					&	6.52	\\			
-		dBSE(TDA)@{\GOWO}@HF	&	7.51					&	6.11	\\			
-		FCI						&	7.14					&	5.47	\\			
-		\end{tabular} 
-	\end{ruledtabular}
-\end{table}
+%\begin{table}
+%	\caption{
+%	Excitation energies (in eV) of CN3 obtained with the aug-cc-pVDZ basis set  at various levels of theory.
+%	%$\Eg^{\GW} = 13.79$ eV.		
+%	\label{tab:CN3}
+%	}
+%	\begin{ruledtabular}
+%		\begin{tabular}{lcc}
+%							&	\mc{2}{c}{Excitation}	\\
+%		Method				&	$^1B_2(\pi \ra \pis)$	&	$^3B_2(\pi \ra \pis)$		\\
+%		\hline
+%		BSE@{\GOWO}@HF			&	7.66					&	6.52	\\			
+%		dBSE(TDA)@{\GOWO}@HF	&	7.51					&	6.11	\\			
+%		FCI						&	7.14					&	5.47	\\			
+%		\end{tabular} 
+%	\end{ruledtabular}
+%\end{table}
 
 %%%%%%%%%%%%%%%%%%%%%%%%
 \section{Conclusion}
@@ -805,9 +812,9 @@ Funding from the \textit{``Centre National de la Recherche Scientifique''} is ac
 This work has also been supported through the EUR grant NanoX ANR-17-EURE-0009 in the framework of the \textit{``Programme des Investissements d'Avenir''.}}
 
 %%%%%%%%%%%%%%%%%%%%%%%%
-\section*{Supporting Information}
+%\section*{Supporting Information}
 %%%%%%%%%%%%%%%%%%%%%%%%
-See {\SI} for plenty of stuff
+%See {\SI} for plenty of stuff
 
 \bibliography{BSEdyn}