SRGGW/Poster/main.tex

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\title{\parbox{0.7\linewidth}{\centering A similarity renormalization group approach to Green's function methods}}
% \title{A similarity renormalization group approach \\ to Green's function methods}
\author{Antoine MARIE and Pierre-François \textsc{LOOS}}
\date{\today}
\institute{Laboratoire de Chimie et Physique Quantiques (UMR 5626), Université de Toulouse, CNRS, UPS, France}

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\newcommand{\bSig}{\boldsymbol{\Sigma}}
\newcommand{\bSigC}{\boldsymbol{\Sigma}^{\text{c}}}
\newcommand{\be}{\boldsymbol{\epsilon}}
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\newcommand{\ii}{\mathrm{i}}
\newcommand{\GW}{GW}
\newcommand{\GF}{\text{GF(2)}}
\newcommand{\GT}{GT}	
\newcommand{\evGW}{\text{ev}GW}	
\newcommand{\qsGW}{\text{qs}GW}
\newcommand{\SRGGW}{\text{SRG-}GW}
\newcommand{\SRGqsGW}{\text{SRG-qs}GW}
\newcommand{\GOWO}{G_0W_0}

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\begin{document}

\maketitle

\begin{columns}
    \column{0.5}
    \block{Dynamic $GW$}
    {
    \begin{minipage}{0.4\linewidth}
      \begin{tikzfigure}
        \includegraphics[width=0.8\textwidth]{square}
      \end{tikzfigure}
    \end{minipage}
    \begin{minipage}{0.6\linewidth}
      \begin{equation*}
	\qty[ \underbrace{\blue{\boldsymbol{F}}}_{\text{\blue{Fock matrix}}} + \underbrace{\violet{\boldsymbol{\Sigma}^{\GW}} (\omega = \teal{\epsilon^{GW}_{p}})}_{\text{\violet{dynamic self-energy}}} ] \psi_{p}^{GW} 
	 = \teal{\epsilon^{GW}_{p}} \psi_{p}^{GW}
       \end{equation*}
       \vspace{1cm}
       \begin{equation*}
         \begin{split}
	\violet{\Sigma_{pq}^{GW}}(\omega) 
			&= \sum_{i\nu} \frac{\red{W_{pi}^{\nu}} \red{W_{qi}^{\nu}}}{\omega - \teal{\epsilon^{GW}_{i}} + \orange{\Omega_{\nu}} - \ii \eta} \\
           &+ \sum_{a\nu} \frac{\red{W_{pa}^{\nu}} \red{W_{qa}^{\nu}}}{\omega - \teal{\epsilon^{GW}_{a}} - \orange{\Omega_{\nu}} + \ii \eta}
         \end{split}
       \end{equation*}
     \end{minipage}
     
     \vspace{0.5cm}
     \small L. Hedin, Phys. Rev. 139, A796 (1965); R. M. Martin, L. Reining, and D. M. Ceperley, (Cambridge University Press, 2016)
    }
    \column{0.5}
    \block{Similarity Renormalization Group (SRG)}{
    \begin{minipage}{0.49\linewidth}
   SRG flow equation
    \begin{equation}
        \label{eq:flowEquation}
        \dv{\boldsymbol{H}(s)}{s} = \comm{\boldsymbol{\eta}(s)}{\boldsymbol{H}(s)}
    \end{equation}
    Similarity transformed Hamiltonian
    \begin{equation}
        \label{eq:SRG_Ham}
        \boldsymbol{H}(s) = \boldsymbol{U}(s) \, \boldsymbol{H} \, \boldsymbol{U}^\dagger(s)
    \end{equation}
    Wegner generator
    %\begin{equation}
    %    \boldsymbol{\eta}(s) = \dv{\boldsymbol{U}(s)}{s}	\boldsymbol{U}^\dagger(s)	= - \boldsymbol{\eta}^\dag(s)
    %\end{equation}
    \begin{equation}
  \boldsymbol{\eta}^\text{W}(s) = \comm{\boldsymbol{H}^\text{d}(s)}{\boldsymbol{H}^\text{od}(s)}
\end{equation}

\vspace{0.5cm}
\small F. Wegner, Ann. Phys. 3, 77 (1994) \\
S. D. Głazek and K. G. Wilson, Phys. Rev. D 48, 5863 (1993)
    \end{minipage}
    \hfill\vline\hfill
    \begin{minipage}{0.49\linewidth}
      \begin{tikzfigure}
        \includegraphics[width=1.\textwidth]{SRGMatrix}
      \end{tikzfigure}
    \end{minipage}
    }
\end{columns}

\begin{columns}
  \column{0.35}
  \block{Static $GW$}
  {
    \begin{tikzfigure}
      \includegraphics[width=0.27\textwidth]{upfolding.pdf}
    \end{tikzfigure}
  \small S. J. Bintrim and T. C. Berkelbach, J. Chem. Phys. 154, 041101
(2021).}
  \column{0.65}
  \block{SRG-$GW$}
  {
    \begin{minipage}{0.6\linewidth}
      \begin{equation*}
        \begin{split}
  	  \blue{\widetilde{\boldsymbol{F}}_{pq}}(s) &= \delta_{pq} \blue{\epsilon^{\text{HF}}_{p}} + \sum_{r\nu} \frac{\Delta_{pr}^{\nu} + \Delta_{qr}^{\nu}}{(\Delta_{pr}^{\nu})^2 + (\Delta_{qr}^{\nu})^2 } \red{W_{pr}^{\nu}} \red{W_{qr}^{\nu}} \qty[1  - e^{-((\Delta_{pr}^{\nu})^2+(\Delta_{qr}^{\nu})^2) s} ] \\
          \\
          \Delta_{pr}^{\nu} &= \teal{\epsilon^{GW}_{p}} - \teal{\epsilon^{GW}_{r}} \pm \orange{\Omega_{\nu}} \\
          \\
          \violet{\widetilde{\Sigma}_{pq}^{\SRGGW}} &= \sum_{i\nu} \frac{e^{-(\Delta_{pi}^{\nu})^2 s}\red{W_{pi}^{\nu}} \red{W_{qi}^{\nu}}e^{-(\Delta_{qi}^{\nu})^2 s}}{\omega - \teal{\epsilon^{GW}_{i}} + \orange{\Omega_{\nu}}} + \sum_{a\nu} \frac{e^{-(\Delta_{pa}^{\nu})^2 s}\red{W_{pa}^{\nu}} \red{W_{qa}^{\nu}}e^{-(\Delta_{qa}^{\nu})^2 s}}{\omega - \teal{\epsilon^{GW}_{a}} - \orange{\Omega_{\nu}}}
        \end{split}
      \end{equation*}
    \end{minipage}
    \begin{minipage}{0.4\linewidth}
      \begin{tikzfigure}
        \includegraphics[width=\textwidth]{fig1.pdf}
      \end{tikzfigure}
    \end{minipage}
  }
  
\end{columns}

\block{Functional form of the qs$GW$ and SRG-qs$GW$}
{
  \begin{adjustbox}{valign=t}
    \begin{minipage}[t]{0.25\linewidth}
      \begin{tikzfigure}
        \includegraphics[width=0.82\textwidth]{fig2a.pdf}
      \end{tikzfigure}
    \end{minipage}
  \end{adjustbox}
  \begin{minipage}[t]{0.5\linewidth}
    \begin{itemize}
    \bigskip
    \item qs$GW$ self-energy:
    \bigskip
    \begin{equation*}
        \boldsymbol{\Sigma}^{\text{qs}GW}_{pq}(\eta) = 
        \sum_{r\nu} \frac{1}{2}\qty(\frac{\Delta_{pr}^{\nu}}{(\Delta_{pr}^{\nu})^2 + \eta^2 } + \frac{\Delta_{qr}^{\nu}}{(\Delta_{qr}^{\nu})^2 + \eta^2}) W_{pr}^{\nu} W_{qr}^{\nu}
    \end{equation*}
    \bigskip
    {\small S. V. Faleev, M. van Schilfgaarde, and T. Kotani, Phys. Rev. Lett. 93, 126406 (2004)}
    \bigskip
    \item SRG-qs$GW$ self-energy:
    \bigskip
    \begin{equation*}
        \boldsymbol{\Sigma}^{\text{SRG-qs}GW}_{pq}(s) = 
        \sum_{r\nu} \frac{\Delta_{pr}^{\nu} + \Delta_{qr}^{\nu}}{(\Delta_{pr}^{\nu})^2 + (\Delta_{qr}^{\nu})^2 } W_{pr}^{\nu} W_{qr}^{\nu} \qty[1  - e^{-((\Delta_{pr}^{\nu})^2+(\Delta_{qr}^{\nu})^2) s} ]
    \end{equation*}
    \bigskip
    {\small A. Marie and P.-F. Loos, arXiv:2303.05984 (2023)}
    \end{itemize}
    \bigskip
  \end{minipage}
  \begin{adjustbox}{valign=t}
    \begin{minipage}[t]{0.25\linewidth}
      \begin{tikzfigure}
        \includegraphics[width=0.82\textwidth]{fig2b.pdf}
      \end{tikzfigure}
    \end{minipage}
  \end{adjustbox}
%  \begin{minipage}[t]{0.26\linewidth}
%    \vspace{3cm}
%    \begin{equation*}
%      \begin{split}
%        &\boldsymbol{\Sigma}^{\text{SRG-qs}GW}_{pq}(s) = \\
%        \\
%        &\sum_{r\nu} \frac{\Delta_{pr}^{\nu} + \Delta_{qr}^{\nu}}{(\Delta_{pr}^{\nu})^2 + (\Delta_{qr}^{\nu})^2 } W_{pr}^{\nu} W_{qr}^{\nu} \qty[1  - e^{-((\Delta_{pr}^{\nu})^2+(\Delta_{qr}^{\nu})^2) s} ]
%      \end{split}
%    \end{equation*}
%  \end{minipage}
}

\begin{columns}
    \column{0.33}
    \block{IP flow parameter dependence}{
        \begin{tikzfigure}
            \includegraphics[height=13.5cm]{fig3.pdf}
          \end{tikzfigure}}
    \column{0.33}
    \block{EA flow parameter dependence}{
        \begin{tikzfigure}
            \includegraphics[height=13.5cm]{fig4.pdf}
        \end{tikzfigure}}
    \column{0.33}
    \block{MAE flow parameter dependence}{    
        \begin{tikzfigure}
            \includegraphics[height=13.5cm]{fig6.pdf}
        \end{tikzfigure}}

    \end{columns}
    

\begin{columns}
    \column{0.85}
\block{$GW$50 statistics}{    
        \begin{tikzfigure}
            \includegraphics[height=13.5cm]{fig5.pdf}
        \end{tikzfigure}}
\column{0.15}
\block{Funding}{    
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).}
\end{columns}

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\end{document}