MRGW
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Manuscript/MRGW.bib
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Manuscript/MRGW.bib
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Manuscript/MRGW.tex
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Manuscript/MRGW.tex
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\documentclass[aip,jcp,reprint,noshowkeys,superscriptaddress,onecolumn]{revtex4-1}
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\usepackage{graphicx,dcolumn,bm,xcolor,microtype,multirow,amscd,amsmath,amssymb,amsfonts,physics,longtable,wrapfig,txfonts,siunitx}
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\usepackage[version=4]{mhchem}
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\usepackage[utf8]{inputenc}
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\usepackage[T1]{fontenc}
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\usepackage{txfonts}
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\usepackage[
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colorlinks=true,
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citecolor=blue,
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breaklinks=true
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]{hyperref}
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\urlstyle{same}
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\newcommand{\ie}{\textit{i.e.}}
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\newcommand{\eg}{\textit{e.g.}}
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\newcommand{\alert}[1]{\textcolor{red}{#1}}
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\usepackage[normalem]{ulem}
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\newcommand{\titou}[1]{\textcolor{red}{#1}}
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\newcommand{\trashPFL}[1]{\textcolor{r\ed}{\sout{#1}}}
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\newcommand{\PFL}[1]{\titou{(\underline{\bf PFL}: #1)}}
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\newcommand{\mc}{\multicolumn}
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\newcommand{\fnm}{\footnotemark}
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\newcommand{\fnt}{\footnotetext}
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\newcommand{\tabc}[1]{\multicolumn{1}{c}{#1}}
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\newcommand{\QP}{\textsc{quantum package}}
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\newcommand{\T}[1]{#1^{\intercal}}
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% coordinates
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\newcommand{\br}{\boldsymbol{r}}
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\newcommand{\bx}{\boldsymbol{x}}
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\newcommand{\dbr}{d\br}
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\newcommand{\dbx}{d\bx}
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% methods
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\newcommand{\GW}{\text{$GW$}}
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\newcommand{\evGW}{ev$GW$}
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\newcommand{\qsGW}{qs$GW$}
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\newcommand{\GOWO}{$G_0W_0$}
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\newcommand{\Hxc}{\text{Hxc}}
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\newcommand{\xc}{\text{xc}}
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\newcommand{\Ha}{\text{H}}
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\newcommand{\co}{\text{c}}
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\newcommand{\x}{\text{x}}
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\newcommand{\KS}{\text{KS}}
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\newcommand{\HF}{\text{HF}}
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\newcommand{\RPA}{\text{RPA}}
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%
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\newcommand{\Ne}{N}
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\newcommand{\Norb}{K}
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\newcommand{\Nocc}{O}
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\newcommand{\Nvir}{V}
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% operators
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\newcommand{\hH}{\Hat{H}}
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\newcommand{\hS}{\Hat{S}}
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% energies
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\newcommand{\Enuc}{E^\text{nuc}}
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\newcommand{\Ec}[1]{E_\text{c}^{#1}}
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\newcommand{\EHF}{E^\text{HF}}
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% orbital energies
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\newcommand{\eps}[2]{\epsilon_{#1}^{#2}}
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\newcommand{\reps}[2]{\Tilde{\epsilon}_{#1}^{#2}}
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\newcommand{\Om}[2]{\Omega_{#1}^{#2}}
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% Matrix elements
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\newcommand{\Sig}[2]{\Sigma_{#1}^{#2}}
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\newcommand{\SigC}[1]{\Sigma^\text{c}_{#1}}
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\newcommand{\rSigC}[1]{\Tilde{\Sigma}^\text{c}_{#1}}
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\newcommand{\SigX}[1]{\Sigma^\text{x}_{#1}}
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\newcommand{\SigXC}[1]{\Sigma^\text{xc}_{#1}}
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\newcommand{\MO}[1]{\phi_{#1}}
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\newcommand{\SO}[1]{\psi_{#1}}
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\newcommand{\ERI}[2]{(#1|#2)}
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\newcommand{\rbra}[1]{(#1|}
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\newcommand{\rket}[1]{|#1)}
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% Matrices
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\newcommand{\bO}{\boldsymbol{0}}
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\newcommand{\bI}{\boldsymbol{1}}
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\newcommand{\bH}{\boldsymbol{H}}
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\newcommand{\bvc}{\boldsymbol{v}}
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\newcommand{\bSig}[1]{\boldsymbol{\Sigma}^{#1}}
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\newcommand{\be}{\boldsymbol{\epsilon}}
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\newcommand{\bOm}[1]{\boldsymbol{\Omega}^{#1}}
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\newcommand{\bA}[2]{\boldsymbol{A}_{#1}^{#2}}
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\newcommand{\bB}[2]{\boldsymbol{B}_{#1}^{#2}}
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\newcommand{\bC}[2]{\boldsymbol{C}_{#1}^{#2}}
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\newcommand{\bD}[2]{\boldsymbol{D}_{#1}^{#2}}
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\newcommand{\bV}[2]{\boldsymbol{V}_{#1}^{#2}}
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\newcommand{\bW}[2]{\boldsymbol{W}_{#1}^{#2}}
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\newcommand{\bX}[2]{\boldsymbol{X}_{#1}^{#2}}
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\newcommand{\bY}[2]{\boldsymbol{Y}_{#1}^{#2}}
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\newcommand{\bZ}[2]{\boldsymbol{Z}_{#1}^{#2}}
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\newcommand{\bc}[2]{\boldsymbol{c}_{#1}^{#2}}
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% orbitals, gaps, etc
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\newcommand{\IP}{I}
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\newcommand{\EA}{A}
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\newcommand{\HOMO}{\text{HOMO}}
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\newcommand{\LUMO}{\text{LUMO}}
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\newcommand{\Eg}{E_\text{g}}
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\newcommand{\EgFun}{\Eg^\text{fund}}
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\newcommand{\EgOpt}{\Eg^\text{opt}}
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\newcommand{\EB}{E_B}
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\newcommand{\RHH}{R_{\ce{H-H}}}
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\newcommand{\ii}{\mathrm{i}}
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% addresses
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\newcommand{\LCPQ}{Laboratoire de Chimie et Physique Quantiques (UMR 5626), Universit\'e de Toulouse, CNRS, UPS, France}
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\begin{document}
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\title{Undressing $GW$ one determinant at a time}
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\author{Pierre-Fran\c{c}ois \surname{Loos}}
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\email{loos@irsamc.ups-tlse.fr}
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\affiliation{\LCPQ}
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\begin{abstract}
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%\bigskip
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%\begin{center}
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% \boxed{\includegraphics[width=0.5\linewidth]{TOC}}
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%\end{center}
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%\bigskip
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\end{abstract}
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\maketitle
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\begin{equation}
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\label{eq:qp_eq}
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\eps{p}{\HF} + \SigC{p}(\omega) - \omega = 0
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\end{equation}
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\begin{equation}
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\label{eq:SigC}
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\SigC{p}(\omega)
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= \sum_{im} \frac{2\ERI{pi}{m}^2}{\omega - \eps{i}{\HF} + \Om{m}{\RPA}}
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+ \sum_{am} \frac{2\ERI{pa}{m}^2}{\omega - \eps{a}{\HF} - \Om{m}{\RPA}}
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\end{equation}
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\begin{equation}
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\ERI{pq}{m} = \sum_{ia} \ERI{pq}{ia} X_{ia,m}^\RPA
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\end{equation}
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\begin{equation}
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\bA{}{\RPA} \cdot \bX{m}{\RPA} = \Om{m}{\RPA} \bX{m}{\RPA}
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\end{equation}
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\begin{equation}
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A_{ia,jb}^{\RPA} = (\eps{a}{\HF} - \eps{i}{\HF}) \delta_{ij} \delta_{ab} + \ERI{ia}{bj}
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\end{equation}
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\begin{equation}
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\ERI{pq}{ia} = \iint \MO{p}(\br_1) \MO{q}(\br_1) \frac{1}{\abs{\br_1 - \br_2}} \MO{i}(\br_2) \MO{a}(\br_2) d\br_1 \dbr_2
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\end{equation}
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\begin{equation}
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\label{eq:Z}
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0 \le Z_{p,s} = \qty[ 1 - \eval{\pdv{\SigC{p}(\omega)}{\omega}}_{\omega = \eps{p,s}{\GW}} ]^{-1} \le 1
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\end{equation}
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\begin{align}
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\sum_{s} Z_{p,s} & = 1
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&
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\sum_{s} Z_{p,s} \eps{p,s}{\GW} & = \eps{p}{\HF}
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\end{align}
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\begin{equation}
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\bH^{(p)} \cdot \bc{}{(p,s)} = \eps{p,s}{\GW} \bc{}{(p,s)}
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\end{equation}
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\begin{equation}
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\label{eq:Hp}
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\bH^{(p)} =
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\begin{pmatrix}
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\eps{p}{\HF} & \bV{p}{\text{2h1p}} & \bV{p}{\text{2p1h}}
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\\
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\T{(\bV{p}{\text{2h1p}})} & \bC{}{\text{2h1p}} & \bO
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\\
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\T{(\bV{p}{\text{2p1h}})} & \bO & \bC{}{\text{2p1h}}
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\end{pmatrix}
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\end{equation}
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\begin{align}
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C^\text{2h1p}_{ija,kcl} & = \qty[ \qty( \eps{i}{\HF} + \eps{j}{\HF} - \eps{a}{\HF}) \delta_{jl} \delta_{ac} - 2 \ERI{ja}{cl} ] \delta_{ik}
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\\
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C^\text{2p1h}_{iab,kcd} & = \qty[ \qty( \eps{a}{\HF} + \eps{b}{\HF} - \eps{i}{\HF}) \delta_{ik} \delta_{ac} + 2 \ERI{ai}{kc} ] \delta_{bd}
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\end{align}
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\begin{align}
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V^\text{2h1p}_{p,klc} & = \sqrt{2} \ERI{pk}{cl}
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&
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V^\text{2p1h}_{p,kcd} & = \sqrt{2} \ERI{pd}{kc}
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\end{align}
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\begin{equation}
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\det[ \bH^{(p)} - \omega \bI ] = 0
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\end{equation}
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\begin{equation}
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\SigC{p}(\omega)
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= \bV{p}{\text{2h1p}} \cdot \qty(\omega \bI - \bC{}{\text{2h1p}} )^{-1} \cdot \T{\qty(\bV{p}{\text{2h1p}})}
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+ \bV{p}{\text{2p1h}} \cdot \qty(\omega \bI - \bC{}{\text{2p1h}} )^{-1} \cdot \T{\qty(\bV{p}{\text{2p1h}})}
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\end{equation}
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\begin{equation}
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\label{eq:Z_proj}
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Z_{p,s} = \qty[ c_{1}^{(p,s)} ]^{2}
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\end{equation}
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\begin{equation}
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\label{eq:Hp}
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\bH^{(P,QIA)} =
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\begin{pmatrix}
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\eps{P}{\HF} & W_{P,QIA} & \bW{P}{\text{2h1p}} & \bW{P}{\text{2p1h}}
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\\
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W_{QIA,P} & D_{QIA,QIA} & \bD{QIA}{\text{2h1p}} & \bD{QIA}{\text{2p1h}}
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\\
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\T{(\bW{P}{\text{2h1p}})} & \T{(\bD{QIA}{\text{2h1p}})} & \bD{}{\text{2h1p}} & \bO
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\\
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\T{(\bW{P}{\text{2p1h}})} & \T{(\bD{QIA}{\text{2p1h}})} & \bO & \bD{}{\text{2p1h}}
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\end{pmatrix}
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\end{equation}
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with
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\begin{gather}
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W_{P,QIA} = \sqrt{2} \ERI{PQ}{IA}
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\\
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D_{QIA,QIA} = \text{sgn}(\eps{Q}{\HF} - \mu) \qty[ \qty(\eps{Q}{\HF} + \eps{A}{\HF} - \eps{I}{\HF} ) + 2 \ERI{IA}{IA} ]
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\\
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D_{QIA,klc}^\text{2h1p} = - 2 \ERI{IA}{cl} \delta_{Qk}
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\\
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D_{QIA,klc}^\text{2p1h} = + 2 \ERI{IA}{kc} \delta_{Qd}
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\end{gather}
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\begin{equation}
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\label{eq:Hp}
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\bH^{(P,QIA)} =
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\begin{pmatrix}
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\eps{P}{\HF} + \SigC{P}(\omega) & W_{P,QIA} + \SigC{P,QIA}(\omega)
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\\
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W_{QIA,P} + \SigC{QIA,P}(\omega) & D_{QIA,QIA} + \SigC{QIA}(\omega)
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\\
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\end{pmatrix}
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\end{equation}
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with
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\begin{align}
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\SigC{P}(\omega)
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& = \bW{P}{\text{2h1p}} \cdot \qty(\omega \bI - \bD{}{\text{2h1p}} )^{-1} \cdot \T{\qty(\bW{P}{\text{2h1p}})}
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+ \bW{P}{\text{2p1h}} \cdot \qty(\omega \bI - \bD{}{\text{2p1h}} )^{-1} \cdot \T{\qty(\bW{P}{\text{2p1h}})}
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\\
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\SigC{QIA}(\omega)
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& = \bD{QIA}{\text{2h1p}} \cdot \qty(\omega \bI - \bD{}{\text{2h1p}} )^{-1} \cdot \T{\qty(\bD{QIA}{\text{2h1p}})}
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+ \bD{QIA}{\text{2p1h}} \cdot \qty(\omega \bI - \bD{}{\text{2p1h}} )^{-1} \cdot \T{\qty(\bD{QIA}{\text{2p1h}})}
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\\
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\SigC{P,QIA}(\omega)
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& = \bW{P}{\text{2h1p}} \cdot \qty(\omega \bI - \bD{}{\text{2h1p}} )^{-1} \cdot \T{\qty(\bD{QIA}{\text{2h1p}})}
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+ \bW{P}{\text{2p1h}} \cdot \qty(\omega \bI - \bD{}{\text{2p1h}} )^{-1} \cdot \T{\qty(\bD{QIA}{\text{2p1h}})}
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\\
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\SigC{QIA,P}(\omega)
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& = \bD{QIA}{\text{2h1p}} \cdot \qty(\omega \bI - \bD{}{\text{2h1p}} )^{-1} \cdot \T{\qty(\bW{P}{\text{2h1p}})}
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+ \bD{QIA}{\text{2p1h}} \cdot \qty(\omega \bI - \bD{}{\text{2p1h}} )^{-1} \cdot \T{\qty(\bW{P}{\text{2p1h}})}
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\end{align}
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%%%%%%%%%%%%%%%%%%%%%%%%
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\acknowledgements{
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This project has received funding from the European Research Council (ERC) under the European Union's Horizon 2020 research and innovation programme (Grant agreement No.~863481).}
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%%%%%%%%%%%%%%%%%%%%%%%%
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section*{Data availability statement}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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The data that supports the findings of this study are available within the article.% and its supplementary material.
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%%%%%%%%%%%%%%%%%%%%%%%%
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\bibliography{MRGW}
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%%%%%%%%%%%%%%%%%%%%%%%%
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\end{document}
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