saving work
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@ -43,6 +43,7 @@
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\newcommand{\HF}{\text{HF}}
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\newcommand{\RPA}{\text{RPA}}
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\newcommand{\BSE}{\text{BSE}}
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\newcommand{\dBSE}{\text{dBSE}}
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\newcommand{\GW}{GW}
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\newcommand{\stat}{\text{stat}}
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\newcommand{\dyn}{\text{dyn}}
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160
sfBSE.tex
160
sfBSE.tex
@ -204,9 +204,165 @@ for the spin-conserved excitations and
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for the spin-flip excitations.
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%================================
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\subsection{The dynamical Bethe-Salpeter equation correction}
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\subsection{Dynamical correction}
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%================================
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\begin{multline}
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\widetilde{W}_{p_\sig q_\sig,r_\sigp s_\sigp}(\omega) = \ERI{p_\sig q_\sig}{r_\sigp s_\sigp}
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+ \sum_m \ERI{p_\sig q_\sig}{m}\ERI{r_\sigp s_\sigp}{m}
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\\
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\times \qty[ \frac{1}{\omega - (\e{s_\sigp}{} - \e{q_\sig}{}) - \Om{m}{\spc,\RPA} + i \eta} + \frac{1}{\omega - (\e{r_\sigp}{} - \e{p_\sig}{}) - \Om{m}{\spc,\RPA} + i \eta} ]
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\end{multline}
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\begin{equation}
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\label{eq:LR-dyn}
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\begin{pmatrix}
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\bA{}{\dBSE}(\omega) & \bB{}{\dBSE}(\omega)
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\\
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-\bB{}{\dBSE}(-\omega) & -\bA{}{\dBSE}(-\omega)
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\\
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\end{pmatrix}
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\cdot
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\begin{pmatrix}
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\bX{m}{\dBSE} \\
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\bY{m}{\dBSE} \\
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\end{pmatrix}
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=
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\Om{m}{\dBSE}
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\begin{pmatrix}
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\bX{m}{\dBSE} \\
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\bY{m}{\dBSE} \\
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\end{pmatrix}
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\end{equation}
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\begin{subequations}
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\begin{align}
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\label{eq:LR_dBSE-A}
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\A{i_\sig a_\tau,j_\sigp b_\taup}{\dBSE}(\omega) & = \A{i_\sig a_\tau,j_\sigp b_\taup}{\RPA} - \delta_{\sig \sigp} \widetilde{W}_{i_\sig j_\sigp,b_\taup a_\tau}(\omega)
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\\
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\label{eq:LR_dBSE-B}
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\B{i_\sig a_\tau,j_\sigp b_\taup}{\dBSE}(\omega) & = \B{i_\sig a_\tau,j_\sigp b_\taup}{\RPA} - \delta_{\sig \sigp} \widetilde{W}_{i_\sig b_\taup,j_\sigp a_\tau}(\omega)
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\end{align}
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\end{subequations}
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\begin{multline}
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\label{eq:LR-PT}
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\begin{pmatrix}
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\bA{}{\dBSE}(\omega) & \bB{}{\dBSE}(\omega) \\
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-\bB{}{\dBSE}(-\omega) & -\bA{}{\dBSE}(-\omega) \\
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\end{pmatrix}
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\\
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=
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\begin{pmatrix}
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\bA{}{(0)} & \bB{}{(0)}
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\\
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-\bB{}{(0)} & -\bA{}{(0)}
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\\
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\end{pmatrix}
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+
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\begin{pmatrix}
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\bA{}{(1)}(\omega) & \bB{}{(1)}(\omega) \\
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-\bB{}{(1)}(-\omega) & -\bA{}{(1)}(-\omega) \\
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\end{pmatrix}
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\end{multline}
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with
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\begin{subequations}
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\begin{align}
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\label{eq:BSE-A0}
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\A{i_\sig a_\tau,j_\sigp b_\taup}{(0)} & = \A{i_\sig a_\tau,j_\sigp b_\taup}{\BSE}
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\\
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\label{eq:BSE-B0}
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\B{i_\sig a_\tau,j_\sigp b_\taup}{(0)} & = \B{i_\sig a_\tau,j_\sigp b_\taup}{\BSE}
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\end{align}
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\end{subequations}
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and
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\begin{subequations}
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\begin{align}
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\label{eq:BSE-A1}
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\A{i_\sig a_\tau,j_\sigp b_\taup}{(1)}(\omega) & = - \delta_{\sig \sigp} \widetilde{W}_{i_\sig j_\sigp,b_\taup a_\tau}(\omega) + \delta_{\sig \sigp} W^{\stat}_{i_\sig j_\sigp,b_\taup a_\tau}
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\\
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\label{eq:BSE-B1}
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\B{i_\sig a_\tau,j_\sigp b_\taup}{(1)}(\omega) & = - \delta_{\sig \sigp} \widetilde{W}_{i_\sig b_\taup,j_\sigp a_\tau}(\omega) + \delta_{\sig \sigp} W^{\stat}_{i_\sig b_\taup,j_\sigp a_\tau}
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\end{align}
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\end{subequations}
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\begin{subequations}
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\begin{gather}
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\Om{m}{\dBSE} = \Om{m}{(0)} + \Om{m}{(1)} + \ldots
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\\
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\begin{pmatrix}
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\bX{m}{\dBSE} \\
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\bY{m}{\dBSE} \\
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\end{pmatrix}
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=
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\begin{pmatrix}
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\bX{m}{(0)} \\
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\bY{m}{(0)} \\
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\end{pmatrix}
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+
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\begin{pmatrix}
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\bX{m}{(1)} \\
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\bY{m}{(1)} \\
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\end{pmatrix}
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+ \ldots
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\end{gather}
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\end{subequations}
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\begin{equation}
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\label{eq:LR-BSE-stat}
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\begin{pmatrix}
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\bA{}{(0)} & \bB{}{(0)} \\
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-\bB{}{(0)} & -\bA{}{(0)} \\
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\end{pmatrix}
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\cdot
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\begin{pmatrix}
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\bX{S}{(0)} \\
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\bY{S}{(0)} \\
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\end{pmatrix}
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=
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\Om{m}{(0)}
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\begin{pmatrix}
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\bX{m}{(0)} \\
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\bY{m}{(0)} \\
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\end{pmatrix}
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\end{equation}
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\begin{equation}
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\label{eq:Om1}
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\Om{m}{(1)} =
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\T{\begin{pmatrix}
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\bX{m}{(0)} \\
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\bY{m}{(0)} \\
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\end{pmatrix}}
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\cdot
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\begin{pmatrix}
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\bA{}{(1)}(\Om{m}{(0)}) & \bB{}{(1)}(\Om{m}{(0)}) \\
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-\bB{}{(1)}(-\Om{m}{(0)}) & -\bA{}{(1)}(-\Om{m}{(0)}) \\
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\end{pmatrix}
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\cdot
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\begin{pmatrix}
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\bX{m}{(0)} \\
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\bY{m}{(0)} \\
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\end{pmatrix}
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\end{equation}
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\begin{equation}
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\label{eq:Om1-TDA}
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\Om{S}{(1)} = \T{(\bX{m}{(0)})} \cdot \bA{}{(1)}(\Om{m}{(0)}) \cdot \bX{m}{(0)}
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\end{equation}
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\begin{equation}
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\label{eq:Z}
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Z_{m} = \qty[ 1 - \T{(\bX{m}{(0)})} \cdot \left. \pdv{\bA{}{(1)}(\Om{m}{})}{\Om{S}{}} \right|_{\Om{m}{} = \Om{m}{(0)}} \cdot \bX{m}{(0)} ]^{-1}
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\end{equation}
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\begin{equation}
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\Om{m}{\dBSE} = \Om{m}{(0)} + Z_{m} \Om{m}{(1)}
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\end{equation}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Computational details}
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\label{sec:compdet}
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