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diff --git a/Poster/main.tex b/Poster/main.tex
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--- a/Poster/main.tex
+++ b/Poster/main.tex
@@ -180,7 +180,7 @@ S. D. Głazek and K. G. Wilson, Phys. Rev. D 48, 5863 (1993)
     \hfill\vline\hfill
     \begin{minipage}{0.49\linewidth}
       \begin{tikzfigure}
-        \includegraphics[width=1.1\textwidth]{SRGMatrix}
+        \includegraphics[width=1.\textwidth]{SRGMatrix}
       \end{tikzfigure}
     \end{minipage}
     }
@@ -220,14 +220,21 @@ S. D. Głazek and K. G. Wilson, Phys. Rev. D 48, 5863 (1993)
 
 \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*}
-        \boxed{\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}}
+        \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)}
@@ -235,16 +242,18 @@ S. D. Głazek and K. G. Wilson, Phys. Rev. D 48, 5863 (1993)
     \item SRG-qs$GW$ self-energy:
     \bigskip
     \begin{equation*}
-        \boxed{\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} ]}
+        \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]{0.5\linewidth}
+    \begin{minipage}[t]{0.25\linewidth}
       \begin{tikzfigure}
-        \includegraphics[width=0.82\textwidth]{fig2.pdf}
+        \includegraphics[width=0.82\textwidth]{fig2b.pdf}
       \end{tikzfigure}
     \end{minipage}
   \end{adjustbox}
@@ -291,6 +300,6 @@ S. D. Głazek and K. G. Wilson, Phys. Rev. D 48, 5863 (1993)
 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=left,draw,fill=footer] at (bottomleft) {\Large \textcolor{white}{\textbf{amarie@irsamc.ups-tlse.fr \hspace{50cm} arXiv:2303.05984}} };
+\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} }};
 
 \end{document}