S2 figures
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Manuscript/H2_BHHLYP_S2.pdf
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Manuscript/H2_BHHLYP_S2.pdf
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Manuscript/H2_BSE_S2.pdf
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Manuscript/H2_BSE_S2.pdf
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Manuscript/H2_CIS_S2.pdf
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Manuscript/H2_CIS_S2.pdf
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@ -709,17 +709,20 @@ Remarkably, SF-BSE shows a good agreement with EOM-CCSD for the $\text{F}\,{}^1\
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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.
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%%% FIG 2 %%%
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\begin{figure}
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\includegraphics[width=\linewidth]{H2_CIS.pdf}
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\includegraphics[width=\linewidth]{H2_BHHLYP.pdf}
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\includegraphics[width=\linewidth]{H2_BSE.pdf}
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\begin{figure*}
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\includegraphics[width=0.45\linewidth]{H2_CIS}
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\includegraphics[width=0.45\linewidth]{H2_CIS_S2}
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\includegraphics[width=0.45\linewidth]{H2_BHHLYP}
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\includegraphics[width=0.45\linewidth]{H2_BHHLYP_S2}
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\includegraphics[width=0.45\linewidth]{H2_BSE}
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\includegraphics[width=0.45\linewidth]{H2_BSE_S2}
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\caption{
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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.
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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.
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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.
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All the spin-conserved and spin-flip calculations have been performed with an unrestricted reference.
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The raw data are reported in the {\SI}.
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\label{fig:H2}}
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\end{figure}
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\end{figure*}
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%%% %%% %%%
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%===============================
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