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diff --git a/Manuscript/sfBSE.tex b/Manuscript/sfBSE.tex
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--- a/Manuscript/sfBSE.tex
+++ b/Manuscript/sfBSE.tex
@@ -709,17 +709,20 @@ Remarkably, SF-BSE shows a good agreement with EOM-CCSD for the $\text{F}\,{}^1\
 A similar graph comparing (SF-)dBSE and EOM-CCSD excitation energies can be found in the {\SI} where it is shown that dynamical effects do not affect the present conclusions.
 
 %%% FIG 2 %%%
-\begin{figure}
-	\includegraphics[width=\linewidth]{H2_CIS.pdf}
-	\includegraphics[width=\linewidth]{H2_BHHLYP.pdf}
-	\includegraphics[width=\linewidth]{H2_BSE.pdf}
+\begin{figure*}
+	\includegraphics[width=0.45\linewidth]{H2_CIS}
+	\includegraphics[width=0.45\linewidth]{H2_CIS_S2}
+	\includegraphics[width=0.45\linewidth]{H2_BHHLYP}
+	\includegraphics[width=0.45\linewidth]{H2_BHHLYP_S2}
+	\includegraphics[width=0.45\linewidth]{H2_BSE}
+	\includegraphics[width=0.45\linewidth]{H2_BSE_S2}
 \caption{
-	Excitation energies of the $\text{B}\,{}^1\Sigma_u^+$ (red), $\text{E}\,{}^1\Sigma_g^+$ (black), and $\text{E}\,{}^1\Sigma_g^+$ (blue) states (with respect to the $\text{X}\,{}^1 \Sigma_g^+$ ground state) of \ce{H2} obtained with the cc-pVQZ basis at the (SF-)CIS (top), (SF-)TD-BH\&HLYP (middle), and (SF-)BSE (bottom) levels of theory.  
+	Excitation energies with respect to the $\text{X}\,{}^1 \Sigma_g^+$ ground state (left) and $\expval*{\hS^2}$ (right) of the $\text{B}\,{}^1\Sigma_u^+$ (red), $\text{E}\,{}^1\Sigma_g^+$ (black), and $\text{E}\,{}^1\Sigma_g^+$ (blue) states of \ce{H2} obtained with the cc-pVQZ basis at the (SF-)CIS (top), (SF-)TD-BH\&HLYP (middle), and (SF-)BSE (bottom) levels of theory.  
 	The reference EOM-CCSD excitation energies are represented as solid lines, while the results obtained with and without spin-flip are represented as dashed and dotted lines, respectively.
 	All the spin-conserved and spin-flip calculations have been performed with an unrestricted reference.
 	The raw data are reported in the {\SI}.
 	\label{fig:H2}}
-\end{figure}
+\end{figure*}
 %%% %%% %%% 
 
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