Manu: started my revision. Saving work
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@ -17,6 +17,7 @@
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\usepackage[normalem]{ulem}
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\newcommand{\titou}[1]{\textcolor{red}{#1}}
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\newcommand{\manu}[1]{\textcolor{blue}{#1}}
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\newcommand{\manurev}[1]{\textcolor{red}{#1}}
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\newcommand{\trashPFL}[1]{\textcolor{red}{\sout{#1}}}
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\newcommand{\trashEF}[1]{\textcolor{blue}{\sout{#1}}}
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@ -589,15 +590,30 @@ following ensemble local-density approximation (eLDA) will be employed
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\beq\label{eq:eLDA_corr_fun}
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\E{c}{\bw}[\n{}{}]\approx \int \n{}{}(\br{}) \e{c}{\bw}(\n{}{}(\br{})) d\br{},
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\eeq
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where the ensemble correlation energy per particle
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where the \manurev{\textit{weight-dependent}} ensemble correlation
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energy per particle \manurev{will have the general
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expression}
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\beq\label{eq:decomp_ens_correner_per_part}
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\e{c}{\bw}(\n{}{})=\sum_{K\geq 0}w_K\be{c}{(K)}(\n{}{})
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\e{c}{\bw}(\n{}{})=\sum_{K\geq 0}w_K\be{c}{(K)}(\n{}{}).
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\eeq
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is explicitly \textit{weight dependent}.
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As shown in Sec.~\ref{sec:eDFA}, the latter can be constructed
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from a finite uniform electron gas model.
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\titou{Note that, here, only the correlation part is treated at the KS level while we rely on exact HF exchange.
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\manurev{Note that, at this level of approximation, which is expected to
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be exact for any \textit{uniform}
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system, the
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density-functional correlation components $\be{c}{(K)}(\n{}{})$ are
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weight-\textit{independent}, unlike in the exact theory \cite{Fromager_2020}.
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As discussed further in Sec.~\ref{sec:eDFA}, these components can be
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extracted from a
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finite uniform electron gas model for which density-functional correlation excitation
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energies can be computed.
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}
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\titou{Note also that, here, only the correlation part of the ensemble
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energy is treated at the
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DFT level while we rely on HF exchange.
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This is different from the usual context where both exchange and correlation are treated at the LDA level which gives compensation of errors.}
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\manu{Manu: I changed a bit your sentence. Is this fine? Maybe we should add
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that we are not interested in accurate ensemble energies. Error
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cancellations may occur when computing excitation
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energies, which are the quantities we are truly interested in.}
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The resulting KS-eLDA ensemble energy obtained via Eq.~\eqref{eq:min_with_HF_ener_fun}
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reads
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