Manu: saving work
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@ -544,6 +544,37 @@ c}\left[n_{\bm\gamma^{\bw}}\right]
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\Big\}.
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\nonumber\\
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\eeq
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% Manu's derivation %%%%
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\color{blue}
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Fock operator:\\
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Stationarity condition
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\beq
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&&\sum_{t^\sigma}\Big(f_{p^\sigma\sigma,t^\sigma\sigma}\Gamma^{(K)\sigma}_{t^\sigma
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q^\sigma}-\Gamma^{(K)\sigma}_{p^\sigma
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t^\sigma}f_{t^\sigma\sigma,q^\sigma\sigma}\Big)
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\nonumber\\
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&&=
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f_{p^\sigma\sigma,q^\sigma\sigma}n^{(K)\sigma}_{q^\sigma}-n^{(K)\sigma}_{p^\sigma}f_{p^\sigma\sigma,q^\sigma\sigma}
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\nonumber\\
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&&=
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\eeq
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%%%%%
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\beq
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&&f_{p^\sigma\sigma,q^\sigma\sigma}=\langle\varphi_p^\sigma\vert\hat{h}\vert\varphi_q^\sigma\rangle
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\nonumber\\
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&&+\sum_{L\geq 0}w_L\sum_{\tau}\sum_{r^\tau s^\tau}
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\nonumber\\
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&&\Big(\langle p^\sigma r^\tau\vert
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q^\sigma s^\tau\rangle\Gamma^{(L)\tau}_{r^\tau
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s^\tau}
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-\delta_{\sigma\tau}\langle p^\sigma r^\sigma\vert
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s^\sigma q^\sigma\rangle\Gamma^{(L)\tau}_{r^\tau
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s^\tau}
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\Big)
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\eeq
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\color{black}
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\\
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%%%%%
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Note that this approximation, where the ensemble density matrix is
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optimized from a non-local exchange potential [rather than a local one,
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as expected from Eq.~(\ref{eq:var_ener_gokdft})] is applicable to real
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