diff --git a/Manuscript/Cx_H2.pdf b/Manuscript/Cx_H2.pdf
deleted file mode 100644
index 0b6b1b0..0000000
Binary files a/Manuscript/Cx_H2.pdf and /dev/null differ
diff --git a/Manuscript/Cxw.pdf b/Manuscript/Cxw.pdf
new file mode 100644
index 0000000..67da299
Binary files /dev/null and b/Manuscript/Cxw.pdf differ
diff --git a/Manuscript/FarDFT.tex b/Manuscript/FarDFT.tex
index ca71a03..8b4cfa7 100644
--- a/Manuscript/FarDFT.tex
+++ b/Manuscript/FarDFT.tex
@@ -392,10 +392,9 @@ However, it is important to ensure that the weight-dependent functional does not
 Finally, let us mention that, around $\ew{} = 0$, the behaviour of Eq.~\eqref{eq:Cxw} is linear.
 
 \begin{figure}
-	\includegraphics[width=0.8\linewidth]{Cx_H2}
+	\includegraphics[width=\linewidth]{Cxw}
 	\caption{
-	$\Cx{\ew{}}/\Cx{\ew{}=0}$ as a function of $\ew{}$ [see Eq.~\eqref{eq:Cxw}] for the \ce{H2} molecule at equilibrium bond length and the aug-cc-pVTZ basis set.
-	\titou{T2: Add the same curve for He and stretch H2.}
+	$\Cx{\ew{}}/\Cx{\ew{}=0}$ as a function of $\ew{}$ [see Eq.~\eqref{eq:Cxw}] computed with the aug-cc-pVTZ basis set for the \ce{He} atom (blue) and the \ce{H2} molecule at $\RHH = 1.4$ bohr (red) and $\RHH = 3.7$ bohr (green).
 	\label{fig:Cx_H2}
 	}
 \end{figure}