saving work in results
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@ -544,9 +544,42 @@ This means that the cations used an unrestricted HF reference while the neutral
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\label{sec:results}
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%=================================================================%
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The results section is divided in two parts.
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The first step will be to analyse in depth the behavior of the two static self-energy approximations in a few test cases.
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Then the accuracy of the IP yielded by the Sym and SRG schemes will be statistically gauged over a test set of molecules.
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%%%%%%%%%%%%%%%%%%%%%%
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\subsection{Flow parameter dependence of the SRG/Sym-qs$GW$/GF(2) schemes}
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\label{sec:flow_param_dep}
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%%%%%%%%%%%%%%%%%%%%%%
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%%% FIG 1 %%%
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\begin{figure*}
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\centering
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\includegraphics[width=\linewidth]{fig1.pdf}
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\caption{
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This figure is terrible, I will clean it. I put it here just to start writing the results discussion. Maybe fig 1 with only He and Ne but also the $\eta$ evolution because possible to converge for these molecules. Then figure 2 with H2O and BeO with SRG GW and SRG GF(2).
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\label{fig:fig1}}
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\end{figure*}
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%%% %%% %%% %%%
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%%%%%%%%%%%%%%%%%%%%%%
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\subsection{Comparison of the Sym-qs and SRG-qs approximations}
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\label{sec:SRG_vs_Sym}
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%%%%%%%%%%%%%%%%%%%%%%
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The test set considered in this study is composed of the GW20 set of molecules introduced by Berkelbach \ant{check ref} and co-workers.
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This set is made of the 20 smallest molecules of the GW100 benchmark set.
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We also added the MgO and O3 molecules which are part of GW100 and are known to be difficult to converged for qs$GW$.
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In addition, we considered the Quest 1 and 2 sets which is made of small and medium size organic molecules.
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%=================================================================%
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\section{Conclusion}
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%%%%%%%%%%%%%%%%%%%%%%
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\label{sec:conclusion}
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%=================================================================%
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Here comes the conclusion.
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%%%%%%%%%%%%%%%%%%%%%%%%
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