Manu: saving work
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@ -331,6 +331,16 @@ c}\left[n\right]}{\partial w_K}
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\right|
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\right|
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_{n=n_{\opGamma{\bw}}}.
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_{n=n_{\opGamma{\bw}}}.
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\eeq
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\eeq
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For implementation purposes, we will use in the rest of this work
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(one-electron reduced) density matrices rather than Slater determinants
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as basic variables. If we denote ${\bmg}^{(K)}$
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\beq
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\Gamma_{\mu\nu}^{(K)}=\sum_{p\in (K)}c_{\mu p}c_{\nu p}
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\eeq
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where the summation runs over the spin-orbitals that are occupied in
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$\Phi^{(K)}$.
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%%%%%%%%%%%%%%%
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%%%%%%%%%%%%%%%
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%\subsection{Hybrid GOK-DFT}
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%\subsection{Hybrid GOK-DFT}
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%%%%%%%%%%%%%%%
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%%%%%%%%%%%%%%%
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