diff --git a/Manuscript/EPAWTFT.tex b/Manuscript/EPAWTFT.tex
index c4d6296..e75d624 100644
--- a/Manuscript/EPAWTFT.tex
+++ b/Manuscript/EPAWTFT.tex
@@ -1253,11 +1253,12 @@ However, they are unable to model functions with square-root branch points, whic
 Figure \ref{fig:PadeRMP} illustrates the improvement brought by diagonal (\ie, $d_A = d_B$) Pad\'e approximants as compared to the usual Taylor expansion in the case of the RMP series of the Hubbard dimer for $U/t = 4.5$.
 
 %%%%%%%%%%%%%%%%%
-\begin{figure}
-    \includegraphics[width=\linewidth]{PadeRMP}
+\begin{figure*}
+    \includegraphics[height=0.23\textheight]{PadeRMP35}
+    \includegraphics[height=0.23\textheight]{PadeRMP45}
     \caption{\label{fig:PadeRMP}
-    RMP ground-state energy as a function of $\lambda$ obtained using various resummation techniques at $U/t = 4.5$.}
-\end{figure}
+    RMP ground-state energy as a function of $\lambda$ obtained using various resummation techniques at $U/t = 3.5$ (left) and $U/t = 4.5$ (right).}
+\end{figure*}
 %%%%%%%%%%%%%%%%%
 
 %==========================================%
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