table water
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@ -215,6 +215,66 @@ In the present study, we rely on the recently proposed short-range density-funct
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\end{squeezetable}
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%%% %%% %%%
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%%% TABLE 1 %%%
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\begin{squeezetable}
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\begin{table*}
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\caption{
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Vertical absorption energies $\Ead$ (in eV) of excited states of water for various methods and basis sets.}
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\begin{ruledtabular}{}
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\begin{tabular}{llddddddddddddd}
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& & & \mc{12}{c}{Deviation with respect to TBE}
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\\
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\cline{4-15}
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& & & \mc{3}{c}{exFCI}
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& \mc{3}{c}{exFCI+PBEot}
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& \mc{3}{c}{exFCI+PBE}
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& \mc{3}{c}{exFCI+LDA}
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\\
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\cline{4-6} \cline{7-9} \cline{10-12} \cline{13-15}
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Molecule & Transition & \tabc{TBE} & \tabc{AVDZ} & \tabc{AVTZ} & \tabc{AVQZ}
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& \tabc{AVDZ} & \tabc{AVTZ} & \tabc{AVQZ}
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& \tabc{AVDZ} & \tabc{AVTZ} & \tabc{AVQZ}
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& \tabc{AVDZ} & \tabc{AVTZ} & \tabc{AVQZ}
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\\
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\hline
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Water & \tabc{$1\,^{1}A_1 \ra 1\,^{1}B_1$} & 7.70 & -0.17 & -0.07 &
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& -0.19 & +0.00 &
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& -0.02 & -0.01 &
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& -0.04 & -0.01 &
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\\
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& \tabc{$1\,^{1}A_1 \ra 1\,^{1}A_2$} & 9.47 & -0.15 & -0.06 &
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& +0.03 & +0.01 &
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& +0.00 & +0.00 &
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& -0.03 & +0.00 &
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\\
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& \tabc{$1\,^{1}A_1 \ra 1\,^{1}A_1$} & 9.97 & -0.03 & +0.02 &
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& +0.13 & +0.08 &
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& +0.10 & +0.07 &
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& +0.09 & 0.07 &
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\\
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& \tabc{$1\,^{1}A_1 \ra 3\,^{1}B_1$} & 7.33 & -0.19 & -0.08 &
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& +0.02 & +0.00 &
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& +0.05 & +0.01 &
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& 0.00 & +0.00 &
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\\
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& \tabc{$1\,^{1}A_1 \ra 3\,^{1}A_2$} & 9.30 & -0.16 & -0.06 &
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& +0.04 & +0.02 &
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& +0.07 & +0.03 &
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& +0.03 & 0.03 &
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\\
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& \tabc{$1\,^{1}A_1 \ra 3\,^{1}A_1$} & 9.59 & -0.11 & -0.05 &
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& +0.07 & +0.02 &
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& +0.09 & +0.03 &
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& +0.06 & 0.03 &
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\\
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\end{tabular}
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\end{ruledtabular}
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\end{table*}
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\end{squeezetable}
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%%% %%% %%%
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%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Conclusion}
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\label{sec:ccl}
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