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RapportStage/CSF_RCV.pdf
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RapportStage/CSF_RCV.pdf
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RapportStage/EMP_RHF_R10.pdf
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RapportStage/EMP_RHF_R10.pdf
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@ -554,6 +554,7 @@ We will take the simple case of the M{\o}ller-Plesset partitioning with a restri
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\begin{figure}[h!]
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\begin{figure}[h!]
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\centering
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\centering
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\includegraphics[width=0.45\textwidth]{EMP_RHF_R10.pdf}
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\includegraphics[width=0.45\textwidth]{RHFMiniBasRCV.pdf}
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\includegraphics[width=0.45\textwidth]{RHFMiniBasRCV.pdf}
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\caption{\centering }
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\caption{\centering }
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\label{fig:RHFMiniBasRCV}
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\label{fig:RHFMiniBasRCV}
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@ -563,13 +564,20 @@ Then we will compare the different partitioning using the same basis set. The \a
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\begin{figure}[h!]
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\begin{figure}[h!]
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\centering
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\centering
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\includegraphics[width=0.8\textwidth]{PartitioningRCV.pdf}
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\includegraphics[width=0.7\textwidth]{PartitioningRCV.pdf}
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\caption{\centering }
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\caption{\centering }
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\label{fig:RadiusPartitioning}
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\label{fig:RadiusPartitioning}
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\end{figure}
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\end{figure}
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Puis différence entre $Y_{l0}$ et $P_l(\cos(\theta))$ (CSF). + petit Parler de la possibilité de la base strong coupling avec la citation paola et les polynomes . \\
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Puis différence entre $Y_{l0}$ et $P_l(\cos(\theta))$ (CSF). + petit Parler de la possibilité de la base strong coupling avec la citation paola et les polynomes . \\
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\begin{figure}[h!]
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\centering
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\includegraphics[width=0.7\textwidth]{CSF_RCV.pdf}
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\caption{\centering }
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\label{fig:RadiusCSF}
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\end{figure}
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Différence RHF/UHF, Hamiltonien non-bloc diagonal, coefficients complexe pour R<3/2 \\
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Différence RHF/UHF, Hamiltonien non-bloc diagonal, coefficients complexe pour R<3/2 \\
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Influence de la taille de la base en RHF et UHF \\
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Influence de la taille de la base en RHF et UHF \\
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@ -584,13 +592,6 @@ UHF: CF point = QPT, ESQPT ???
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PT broken symmetry sb UHF
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PT broken symmetry sb UHF
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\section{To do list}
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\begin{itemize}
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\item Corriger les erreurs dans la biblio
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\item citation spin density wave et charge density wave
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\end{itemize}
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\section{Conclusion}
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\section{Conclusion}
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\newpage
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\newpage
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