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Pierre-Francois Loos 2020-01-31 09:59:27 +01:00
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@ -370,6 +370,7 @@ In summary, each method has its own strengths and weaknesses, and none of them i
\begin{figure*}
\includegraphics[width=\linewidth]{QUEST1}
\caption{\hl{Mean absolute error (MAE, top) and mean signed error (MSE, bottom)} with respect to the TBE/\textit{aug}-cc-pVTZ values from the {\SetA} set (as described in Ref.~\citenum{Loo18a}) for various methods and types of excited states.
\hl{The corresponding graph for the maximum positive and negative errors can be found in the} {\SI}.
}
\label{fig:Set1}
\end{figure*}
@ -388,7 +389,9 @@ In summary, each method has its own strengths and weaknesses, and none of them i
%%% FIG 3 %%%
\begin{figure*}
\includegraphics[width=\linewidth]{QUEST3}
\caption{\hl{Mean absolute error (MAE, top) and mean signed error (MSE, bottom)} with respect to the TBE/\textit{aug}-cc-pVTZ values from the {\SetC} set (as described in Ref.~\citenum{Loo20a}) for various methods and types of excited states.}
\caption{\hl{Mean absolute error (MAE, top) and mean signed error (MSE, bottom)} with respect to the TBE/\textit{aug}-cc-pVTZ values from the {\SetC} set (as described in Ref.~\citenum{Loo20a}) for various methods and types of excited states.
\hl{The corresponding graph for the maximum positive and negative errors can be found in the} {\SI}.
}
\label{fig:Set3}
\end{figure*}
%%% %%% %%%