diff --git a/Manuscript/EPAWTFT.tex b/Manuscript/EPAWTFT.tex
index ae2b5a1..7146f0a 100644
--- a/Manuscript/EPAWTFT.tex
+++ b/Manuscript/EPAWTFT.tex
@@ -338,7 +338,6 @@ unless otherwise stated, atomic units will be used throughout.
 	Exact energies for the Hubbard dimer ($U=4t$) as functions of $\lambda$ on the real axis (\subref{subfig:FCI_real}) and in the complex plane (\subref{subfig:FCI_cplx}).
     Only the interacting closed-shell singlets are plotted in the complex plane, becoming degenerate at the EP (black dot).
     The contour followed around the EP in order to interchange states is also represented.
-    \hugh{HUGH TO ADD CONTOUR AGAIN....}
 	\label{fig:FCI}}
 \end{figure*}
 
@@ -1927,7 +1926,7 @@ and applications of perturbation theory.
 
 % DIRECTIONS
 Perturbation theory isn't usually considered in the complex plane. 
-But when it is, we have seen that a lot can be learnt about the performance of perturbation theory on the real axis.
+But when it is, a lot can be learnt about the performance of perturbation theory on the real axis.
 These insights can allow incredibly accurate results to be obtained using only the lowest-order terms in a perturbation series.
 Yet perturbation theory represents only one method for approximating the exact energy, and few other methods
 have been considered through similar complex non-Hermitian extensions.
diff --git a/Manuscript/fig1b.pdf b/Manuscript/fig1b.pdf
index 80d55c4..c1d358a 100644
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