diff --git a/Manuscript/EPAWTFT.tex b/Manuscript/EPAWTFT.tex
index 12416bd..ff5ecf6 100644
--- a/Manuscript/EPAWTFT.tex
+++ b/Manuscript/EPAWTFT.tex
@@ -519,10 +519,11 @@ correctly modelling the physics of the system with the two electrons on opposing
     \end{subfigure}
 	\caption{%
     \hugh{(\subref{subfig:UHF_cplx_angle}) Real component of the UHF angle $\ta^{\text{UHF}}$ for $\lambda \in \bbC$.
-    Symmetry-broken solutions correspond to individual sheets and become equivalent at the quasi-EP $\lambda_{\text{c}}$ (black dot).
+    Symmetry-broken solutions correspond to individual sheets and become equivalent at 
+    the \textit{quasi}-EP $\lambda_{\text{c}}$ (black dot).
     The RHF solution is independent of $\lambda$, giving constant plane at $\pi/2$.
     (\subref{subfig:UHF_cplx_energy}) The corresponding HF energy surfaces show a non-analytic 
-    point at the quasi-exceptional point.}
+    point at the \textit{quasi}-EP.}
 	\label{fig:HF_cplx}}
 \end{figure*}
 %%%%%%%%%%%%%%%%%
@@ -577,7 +578,7 @@ the holomorphic HF approach.\cite{Hiscock_2014,Burton_2016,Burton_2018}
 Remarkably, the coalescence point in this analytic continuation emerges as a 
 \textit{quasi}-EP on the real $\lambda$ axis (Fig.~\ref{fig:HF_cplx}), where
 the different HF solutions become equivalent but not self-orthogonal.\cite{Burton_2019}
-By analogy with perturbation theory, the regime where this quasi-EP occurs 
+By analogy with perturbation theory, the regime where this \textit{quasi}-EP occurs 
 within $\lambda_{\text{c}} \le 1$ can be interpreted as an indication that 
 the symmetry-pure reference orbitals no longer provide a qualitatively 
 accurate representation for the true HF ground state at $\lambda = 1$.
@@ -596,7 +597,7 @@ to an adiabatic connection in density-functional theory,\cite{Langreth_1975,Gunn
 a ground-state wave function can be ``morphed'' into an excited-state wave function 
 via a stationary path of HF solutions.
 This novel approach to identifying excited-state wave functions demonstrates the fundamental 
-role of quasi-EPs in determining the behaviour of the HF approximation.} 
+role of \textit{quasi}-EPs in determining the behaviour of the HF approximation.} 
 
 %\titou{In a recent paper, \cite{Burton_2019} using holomorphic Hartree-Fock (h-HF) \cite{Hiscock_2014,Burton_2018,Burton_2016} as an analytic continuation of conventional HF theory, we have demonstrated, on a simple model, that one can interconvert states of different symmetries and natures by following well-defined contours in the complex $\lambda$-plane, where $\lambda$ is the strength of the electron-electron interaction (see Fig.~\ref{fig:iAC}).
 %In particular, by slowly varying $\lambda$ in a similar (yet different) manner to an adiabatic connection in density-functional theory, \cite{Langreth_1975,Gunnarsson_1976,Zhang_2004} one can ``morph'' a ground-state wave function into an excited-state wave function via a stationary path of HF solutions. \cite{Seidl_2018}