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BSEdyn.tex
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BSEdyn.tex
@ -681,6 +681,7 @@ All the BSE calculations have been performed with our locally developed $GW$ sof
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\caption{
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\caption{
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Singlet excitation energies (in eV) for various molecules obtained with the aug-cc-pVTZ basis set at various levels of theory.
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Singlet excitation energies (in eV) for various molecules obtained with the aug-cc-pVTZ basis set at various levels of theory.
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The dynamical correction is computed in the TDA.
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The dynamical correction is computed in the TDA.
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CT and R stand respectively for charge transfer and Rydberg.
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\label{tab:BigTabSi}
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\label{tab:BigTabSi}
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}
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}
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\begin{ruledtabular}
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\begin{ruledtabular}
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@ -691,7 +692,7 @@ All the BSE calculations have been performed with our locally developed $GW$ sof
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& \tabc{$\Eg^{\GW}$} & \tabc{$\Om{m}{\stat}$} & \tabc{$\Om{m}{\dyn}$} & \tabc{$\Delta\Om{m}{\dyn}$} & \tabc{$Z_{m}$}
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& \tabc{$\Eg^{\GW}$} & \tabc{$\Om{m}{\stat}$} & \tabc{$\Om{m}{\dyn}$} & \tabc{$\Delta\Om{m}{\dyn}$} & \tabc{$Z_{m}$}
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& \tabc{CIS(D)} & \tabc{ADC(2)} & \tabc{CCSD} & \tabc{CC2} & \tabc{CC3} \\
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& \tabc{CIS(D)} & \tabc{ADC(2)} & \tabc{CCSD} & \tabc{CC2} & \tabc{CC3} \\
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\hline
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\hline
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\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 \\
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\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 \\
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\\
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\\
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\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 \\
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\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 \\
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& $^1A_2(n \ra 3p)$ & & 9.79 & 9.72 & -0.07 & 1.005 & & & & & & 9.41 & 8.84 & 9.36 & 8.89 & 9.43 \\
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& $^1A_2(n \ra 3p)$ & & 9.79 & 9.72 & -0.07 & 1.005 & & & & & & 9.41 & 8.84 & 9.36 & 8.89 & 9.43 \\
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@ -712,9 +713,12 @@ All the BSE calculations have been performed with our locally developed $GW$ sof
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& $^1\Sigma^+$(R) & & 12.39 & 12.37 & -0.02 & 1.003 & & & & & & 11.71 & 11.83 & 11.75 & 11.63 & 11.49 \\
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& $^1\Sigma^+$(R) & & 12.39 & 12.37 & -0.02 & 1.003 & & & & & & 11.71 & 11.83 & 11.75 & 11.63 & 11.49 \\
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& $^1\Pi$(R) & & 12.37 & 12.32 & -0.05 & 1.004 & & & & & & 12.06 & 12.03 & 11.96 & 11.83 & 11.69 \\
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& $^1\Pi$(R) & & 12.37 & 12.32 & -0.05 & 1.004 & & & & & & 12.06 & 12.03 & 11.96 & 11.83 & 11.69 \\
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\\
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\\
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\ce{C2H4} & $^1B_{3u}(\pi \ra 3s)$ & & & & & & & & & & & 7.35 & 7.34 & 7.42 & 7.29 & 7.35 \\
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\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 \\
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& $^1B_{1u}(\pi \ra \pis)$ & & & & & & & & & & & 7.95 & 7.91 & 8.02 & 7.92 & 7.91 \\
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& $^1A'$(R) & & 7.05 & 7.01 & -0.037 & 1.003 & & & & & & 5.81 & 5.73 & 6.30 & 5.72 & 6.26 \\
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& $^1B_{1g}(\pi \ra 3p)$ & & & & & & & & & & & 8.01 & 7.99 & 8.08 & 7.95 & 8.03 \\
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\\
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\ce{C2H4} & $^1B_{3u}(\pi \ra 3s)$ & 11.49 & 7.64 & & & & & & & & & 7.35 & 7.34 & 7.42 & 7.29 & 7.35 \\
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& $^1B_{1u}(\pi \ra \pis)$ & & 8.18 & & & & & & & & & 7.95 & 7.91 & 8.02 & 7.92 & 7.91 \\
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& $^1B_{1g}(\pi \ra 3p)$ & & 8.29 & & & & & & & & & 8.01 & 7.99 & 8.08 & 7.95 & 8.03 \\
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\\
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\\
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\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 \\
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\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 \\
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& $^1B_2(n \ra 3s)$ & & 7.87 & 7.85 & -0.02 & 1.001 & & & & & & 6.64 & 6.50 & 7.23 & 6.56 & 7.18 \\
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& $^1B_2(n \ra 3s)$ & & 7.87 & 7.85 & -0.02 & 1.001 & & & & & & 6.64 & 6.50 & 7.23 & 6.56 & 7.18 \\
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@ -757,7 +761,10 @@ All the BSE calculations have been performed with our locally developed $GW$ sof
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& $^3\Sigma_u^-(\pi \ra \pis)$ & & 10.79 & 10.38 & -0.42 & 1.034 & & & & & & 10.10 & 10.01 & 9.81 & 10.27 & 9.82 \\
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& $^3\Sigma_u^-(\pi \ra \pis)$ & & 10.79 & 10.38 & -0.42 & 1.034 & & & & & & 10.10 & 10.01 & 9.81 & 10.27 & 9.82 \\
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& $^3\Sigma_u^+$(R) & & 11.48 & 11.38 & -0.10 & 1.010 & & & & & & 10.98 & 10.83 & 10.71 & 10.60 & 10.45 \\
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& $^3\Sigma_u^+$(R) & & 11.48 & 11.38 & -0.10 & 1.010 & & & & & & 10.98 & 10.83 & 10.71 & 10.60 & 10.45 \\
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\\
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\\
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\ce{C2H4} & $^3B_{1u}(\pi \ra \pis)$ & & & & & & & & & & & 4.62 & 4.59 & 4.46 & 4.59 & 4.53 \\
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\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 \\
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& $^3A'(\pi \ra \pis)$ & & 6.69 & 6.70 & 0.01 & 1.000 & & & & & & 5.72 & 5.46 & 5.49 & 5.44 & 5.59 \\
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\\
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\ce{C2H4} & $^3B_{1u}(\pi \ra \pis)$ & 11.49 & & & & & & & & & & 4.62 & 4.59 & 4.46 & 4.59 & 4.53 \\
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& $^3B_{3u}(\pi \ra 3s)$ & & & & & & & & & & & 7.26 & 7.23 & 7.29 & 7.19 & 7.24 \\
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& $^3B_{3u}(\pi \ra 3s)$ & & & & & & & & & & & 7.26 & 7.23 & 7.29 & 7.19 & 7.24 \\
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& $^3B_{1g}(\pi \ra 3p)$ & & & & & & & & & & & 7.97 & 7.95 & 8.03 & 7.91 & 7.98 \\
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& $^3B_{1g}(\pi \ra 3p)$ & & & & & & & & & & & 7.97 & 7.95 & 8.03 & 7.91 & 7.98 \\
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\\
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\\
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@ -772,23 +779,23 @@ All the BSE calculations have been performed with our locally developed $GW$ sof
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\end{table*}
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\end{table*}
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%%% TABLE III %%%
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%%% TABLE III %%%
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\begin{table}
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%\begin{table}
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\caption{
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% \caption{
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Excitation energies (in eV) of CN3 obtained with the aug-cc-pVDZ basis set at various levels of theory.
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% Excitation energies (in eV) of CN3 obtained with the aug-cc-pVDZ basis set at various levels of theory.
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%$\Eg^{\GW} = 13.79$ eV.
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% %$\Eg^{\GW} = 13.79$ eV.
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\label{tab:CN3}
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% \label{tab:CN3}
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}
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% }
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\begin{ruledtabular}
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% \begin{ruledtabular}
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\begin{tabular}{lcc}
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% \begin{tabular}{lcc}
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& \mc{2}{c}{Excitation} \\
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% & \mc{2}{c}{Excitation} \\
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Method & $^1B_2(\pi \ra \pis)$ & $^3B_2(\pi \ra \pis)$ \\
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% Method & $^1B_2(\pi \ra \pis)$ & $^3B_2(\pi \ra \pis)$ \\
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\hline
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% \hline
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BSE@{\GOWO}@HF & 7.66 & 6.52 \\
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% BSE@{\GOWO}@HF & 7.66 & 6.52 \\
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dBSE(TDA)@{\GOWO}@HF & 7.51 & 6.11 \\
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% dBSE(TDA)@{\GOWO}@HF & 7.51 & 6.11 \\
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FCI & 7.14 & 5.47 \\
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% FCI & 7.14 & 5.47 \\
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\end{tabular}
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% \end{tabular}
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\end{ruledtabular}
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% \end{ruledtabular}
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\end{table}
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%\end{table}
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%%%%%%%%%%%%%%%%%%%%%%%%
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%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Conclusion}
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\section{Conclusion}
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@ -805,9 +812,9 @@ Funding from the \textit{``Centre National de la Recherche Scientifique''} is ac
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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''.}}
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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''.}}
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%%%%%%%%%%%%%%%%%%%%%%%%
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%%%%%%%%%%%%%%%%%%%%%%%%
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\section*{Supporting Information}
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%\section*{Supporting Information}
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%%%%%%%%%%%%%%%%%%%%%%%%
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%%%%%%%%%%%%%%%%%%%%%%%%
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See {\SI} for plenty of stuff
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%See {\SI} for plenty of stuff
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\bibliography{BSEdyn}
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\bibliography{BSEdyn}
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