saving work in poster

Poster/main.tex

@@ -17,6 +17,39 @@
 \date{\today}
 \institute{Laboratoire de Chimie et Physique Quantiques (UMR 5626), Université de Toulouse, CNRS, UPS, France}
 
+\definecolor{darkgreen}{RGB}{0, 180, 0}
+\definecolor{fooblue}{RGB}{0,153,255}
+\definecolor{fooyellow}{RGB}{234,180,0}
+\definecolor{lavender}{rgb}{0.71, 0.49, 0.86}
+\definecolor{inchworm}{rgb}{0.7, 0.93, 0.36}
+\newcommand{\violet}[1]{\textcolor{violet}{#1}}
+\newcommand{\orange}[1]{\textcolor{orange}{#1}}
+\newcommand{\purple}[1]{\textcolor{purple}{#1}}
+\newcommand{\blue}[1]{\textcolor{blue}{#1}}
+\newcommand{\green}[1]{\textcolor{darkgreen}{#1}}
+\newcommand{\yellow}[1]{\textcolor{fooyellow}{#1}}
+\newcommand{\red}[1]{\textcolor{red}{#1}}
+\newcommand{\cyan}[1]{\textcolor{cyan}{#1}}
+\newcommand{\magenta}[1]{\textcolor{magenta}{#1}}
+\newcommand{\highlight}[1]{\textcolor{fooblue}{#1}}
+\newcommand{\pub}[1]{\textcolor{purple}{#1}}
+
+\newcommand{\bSig}{\boldsymbol{\Sigma}}
+\newcommand{\bSigC}{\boldsymbol{\Sigma}^{\text{c}}}
+\newcommand{\be}{\boldsymbol{\epsilon}}
+\newcommand{\bOm}{\boldsymbol{\Omega}}
+\newcommand{\bEta}[1]{\boldsymbol{\eta}^{(#1)}(s)}
+
+\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}
+
 \makeatletter
 \newcommand\insertlogoi[2][]{\def\@insertlogoi{\includegraphics[#1]{#2}}}
 \newcommand\insertlogoii[2][]{\def\@insertlogoii{\includegraphics[#1]{#2}}}
@@ -92,10 +125,31 @@
 
 \begin{columns}
     \column{0.5}
-    \block{GW}{\blindtext}
+    \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 = \epsilon^{GW}_{p})}_{\text{\violet{dynamic self-energy}}} ] \psi_{p}^{GW} 
+	 = \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 - \epsilon^{GW}_{i} + \orange{\Omega_{\nu}} - \ii \eta} \\
+           &+ \sum_{a\nu} \frac{\red{W_{pa}^{\nu}} \red{W_{qa}^{\nu}}}{\omega - \epsilon^{GW}_{a} - \orange{\Omega_{\nu}} + \ii \eta}
+         \end{split}
+       \end{equation*}	
+     \end{minipage}
+    }
     \column{0.5}
     \block{SRG}{
-    \begin{minipage}[t]{0.48\linewidth}
+    \begin{minipage}{0.49\linewidth}
     The pillar of the SRG formalism is the flow equation
     \begin{equation}
         \label{eq:flowEquation}
@@ -115,61 +169,100 @@
 \end{equation}
     \end{minipage}
     \hfill\vline\hfill
-    \begin{minipage}[t]{0.48\linewidth}
+    \begin{minipage}{0.49\linewidth}
-            BLABLABLA
+      \begin{tikzfigure}
+        \includegraphics[width=0.9\textwidth]{SRGMatrix}
+      \end{tikzfigure}
     \end{minipage}
     }
 \end{columns}
 
-\block{SRG-GW}
-    {
-    \begin{minipage}{0.7\linewidth}
-        \blindtext
-    \end{minipage}
-    \begin{minipage}{0.3\linewidth}
-        \begin{tikzfigure}
-            \includegraphics[width=0.85\textwidth]{fig1.pdf}
-        \end{tikzfigure}
-    \end{minipage}
-    }
-
-    \block{Functional form of the qs$GW$ and SRG-qs$GW$}{
-        \begin{minipage}[t]{0.25\linewidth}
-            BLABLABLA
-        \end{minipage}
-        \begin{adjustbox}{valign=t}
-        \begin{minipage}[t]{0.5\linewidth}
-            \begin{tikzfigure}
-                \includegraphics[width=0.8\textwidth]{fig2.pdf}
-            \end{tikzfigure}
-        \end{minipage}
-        \end{adjustbox}
-        \begin{minipage}[t]{0.25\linewidth}
-            BLABLABLA
-        \end{minipage}
-    }
-
 \begin{columns}
-    \column{0.5}
+  \column{0.35}
-    \block{Something else}{
+  \block{Static $GW$}
-        \begin{tikzfigure}
+  {
-            \includegraphics[height=15cm]{fig3.pdf}
+    \begin{tikzfigure}
-        \end{tikzfigure}}
+      \includegraphics[width=0.29\textwidth]{upfolding.pdf}
-    \column{0.5}
+    \end{tikzfigure}}
-    \block{$GW$50 statistics}{    
+  \column{0.65}
-        \begin{tikzfigure}
+  \block{SRG-$GW$}
-            \includegraphics[height=15cm]{fig6.pdf}
+  {
-        \end{tikzfigure}}
+    \begin{minipage}{0.575\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} ] \\
+	  &\qq{with} \Delta_{pr}^{\nu} = \epsilon^{GW}_{p} - \epsilon^{GW}_{r} \pm \Omega_\nu \\
+          \\
+          &\violet{\widetilde{\Sigma}_{pq}^{\SRGGW}}(\omega;s) = \\
+          &\sum_{i\nu} \frac{\red{W_{pi}^{\nu}} \red{W_{qi}^{\nu}}e^{-((\Delta_{pi}^{\nu})^2+(\Delta_{qi}^{\nu})^2) s}}{\omega - \epsilon^{GW}_{i} + \Omega_{\nu}} + \sum_{a\nu} \frac{\red{W_{pa}^{\nu}} \red{W_{qa}^{\nu}}e^{-((\Delta_{pa}^{\nu})^2+(\Delta_{qa}^{\nu})^2) s}}{\omega - \epsilon^{GW}_{a} - \Omega_{\nu}}
+        \end{split}
+      \end{equation*}
+    \end{minipage}
+    \begin{minipage}{0.425\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{minipage}[t]{0.275\linewidth}
+    \vspace{2.5cm}
+    \begin{equation*}
+      \begin{split}
+        &\boldsymbol{\Sigma}^{\text{qs}GW}_{pq}(\eta) = \delta_{pq} \epsilon^{\text{HF}}_{p} + \\
+        \\
+        &\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{split}
+    \end{equation*}
+  \end{minipage}
+  \begin{adjustbox}{valign=t}
+    \begin{minipage}[t]{0.45\linewidth}
+      \begin{tikzfigure}
+        \includegraphics[width=0.8\textwidth]{fig2.pdf}
+      \end{tikzfigure}
+    \end{minipage}
+  \end{adjustbox}
+  \begin{minipage}[t]{0.275\linewidth}
+    \vspace{2.5cm}
+    \begin{equation*}
+      \begin{split}
+        &\boldsymbol{\Sigma}^{\text{SRG-qs}GW}_{pq}(s) = \delta_{pq} \epsilon^{\text{HF}}_{p} + \\
+        \\
+        &\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=14cm]{fig3.pdf}
+          \end{tikzfigure}}
+    \column{0.33}
+    \block{EA flow parameter dependence}{
+        \begin{tikzfigure}
+            \includegraphics[height=14cm]{fig4.pdf}
+        \end{tikzfigure}}
+    \column{0.33}
+    \block{MAE flow parameter dependence}{    
+        \begin{tikzfigure}
+            \includegraphics[height=14cm]{fig6.pdf}
+        \end{tikzfigure}}
+
+    \end{columns}
+    
 
 \begin{columns}
     \column{0.85}
 \block{$GW$50 statistics}{    
         \begin{tikzfigure}
-            \includegraphics[height=15cm]{fig5.pdf}
+            \includegraphics[height=14cm]{fig5.pdf}
         \end{tikzfigure}}
 \column{0.15}
 \block{Funding}{