add footer, work on second line of boxes

Poster/main.tex

@@ -22,6 +22,7 @@
 \definecolor{fooyellow}{RGB}{234,180,0}
 \definecolor{lavender}{rgb}{0.71, 0.49, 0.86}
 \definecolor{inchworm}{rgb}{0.7, 0.93, 0.36}
+\definecolor{footer}{cmyk}{0.739,0.288,0,0.278}
 \newcommand{\violet}[1]{\textcolor{violet}{#1}}
 \newcommand{\orange}[1]{\textcolor{orange}{#1}}
 \newcommand{\purple}[1]{\textcolor{purple}{#1}}
@@ -151,17 +152,17 @@
     \column{0.5}
     \block{Similarity Renormalization Group (SRG)}{
     \begin{minipage}{0.49\linewidth}
-    The pillar of the SRG formalism is the flow equation
+   SRG flow equation
     \begin{equation}
         \label{eq:flowEquation}
         \dv{\boldsymbol{H}(s)}{s} = \comm{\boldsymbol{\eta}(s)}{\boldsymbol{H}(s)}
     \end{equation}
-    with the similarity transformed Hamiltonian
+    Similarity transformed Hamiltonian
     \begin{equation}
         \label{eq:SRG_Ham}
         \boldsymbol{H}(s) = \boldsymbol{U}(s) \, \boldsymbol{H} \, \boldsymbol{U}^\dagger(s)
     \end{equation}
-    In this work, we use Wegner's generator
+    Wegner generator
     %\begin{equation}
     %    \boldsymbol{\eta}(s) = \dv{\boldsymbol{U}(s)}{s}	\boldsymbol{U}^\dagger(s)	= - \boldsymbol{\eta}^\dag(s)
     %\end{equation}
@@ -172,7 +173,7 @@
     \hfill\vline\hfill
     \begin{minipage}{0.49\linewidth}
       \begin{tikzfigure}
-        \includegraphics[width=0.9\textwidth]{SRGMatrix}
+        \includegraphics[width=1.1\textwidth]{SRGMatrix}
       \end{tikzfigure}
     \end{minipage}
     }
@@ -188,18 +189,17 @@
   \column{0.65}
   \block{SRG-$GW$}
   {
-    \begin{minipage}{0.575\linewidth}
+    \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} ] \\
-	  &\qq{with} \Delta_{pr}^{\nu} = \teal{\epsilon^{GW}_{p}} - \teal{\epsilon^{GW}_{r}} \pm \orange{\Omega_{\nu}} \\
+  	  \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}}(\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 - \teal{\epsilon^{GW}_{i}} + \orange{\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 - \teal{\epsilon^{GW}_{a}} - \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}{0.425\linewidth}
+    \begin{minipage}{0.4\linewidth}
       \begin{tikzfigure}
         \includegraphics[width=\textwidth]{fig1.pdf}
       \end{tikzfigure}
@@ -210,8 +210,8 @@
 
 \block{Functional form of the qs$GW$ and SRG-qs$GW$}
 {
-  \begin{minipage}[t]{0.275\linewidth}
-    \vspace{2.5cm}
+  \begin{minipage}[t]{0.24\linewidth}
+    \vspace{3cm}
     \begin{equation*}
       \begin{split}
         &\boldsymbol{\Sigma}^{\text{qs}GW}_{pq}(\eta) = \\
@@ -221,14 +221,14 @@
     \end{equation*}
   \end{minipage}
   \begin{adjustbox}{valign=t}
-    \begin{minipage}[t]{0.45\linewidth}
+    \begin{minipage}[t]{0.5\linewidth}
       \begin{tikzfigure}
-        \includegraphics[width=0.8\textwidth]{fig2.pdf}
+        \includegraphics[width=0.82\textwidth]{fig2.pdf}
       \end{tikzfigure}
     \end{minipage}
   \end{adjustbox}
-  \begin{minipage}[t]{0.275\linewidth}
-    \vspace{2.5cm}
+  \begin{minipage}[t]{0.26\linewidth}
+    \vspace{3cm}
     \begin{equation*}
       \begin{split}
         &\boldsymbol{\Sigma}^{\text{SRG-qs}GW}_{pq}(s) = \\
@@ -270,7 +270,6 @@
 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}
 
-\node [above right,outer sep=0pt,minimum width=\paperwidth,align=center,draw,fill=blue!30] at (bottomleft) {Blabla};
-
+\node [above right,outer sep=0pt,minimum width=\paperwidth,align=left,draw,fill=footer] at (bottomleft) {\Large \textcolor{white}{\textbf{amarie@irsamc.ups-tlse.fr \hspace{50cm} arXiv:2303.05984}} };
 
 \end{document}