diff --git a/Manuscript/EPAWTFT.tex b/Manuscript/EPAWTFT.tex
index 15fffee..89fb780 100644
--- a/Manuscript/EPAWTFT.tex
+++ b/Manuscript/EPAWTFT.tex
@@ -503,7 +503,7 @@ the total spin operator $\hat{\mathcal{S}}^2$, leading to ``spin-contamination''
 \begin{figure}
     \includegraphics[width=\linewidth]{HF_real.pdf}
     \caption{\label{fig:HF_real}
-    RHF and UHF energies as a function of the correlation strength $U/t$. 
+    RHF and UHF energies \titou{in the Hubbard dimer} as a function of the correlation strength $U/t$. 
     The symmetry-broken UHF solution emerges at the coalescence point $U=2t$ (black dot), often known as the Coulson-Fischer point.}
 \end{figure}
 %%%%%%%%%%%%%%%%%
@@ -553,7 +553,7 @@ modelling the correct physics with the two electrons on opposite sites.
 	\subcaption{\label{subfig:UHF_cplx_energy}}
     \end{subfigure}
 	\caption{%
-    (\subref{subfig:UHF_cplx_angle}) Real component of the UHF angle $\ta^{\text{UHF}}$ for $\lambda \in \bbC$.
+    (\subref{subfig:UHF_cplx_angle}) Real component of the UHF angle $\ta^{\text{UHF}}$ for $\lambda \in \bbC$ \titou{in the Hubbard dimer for $U/t = ??$}.
     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 the constant plane at $\pi/2$.
@@ -629,7 +629,7 @@ In contrast, $U < 2t$ yields $\lambda_{\text{c}} > 1$ and corresponds to
 the regime where the HF ground state is correctly represented by symmetry-pure orbitals.
 
 % COMPLEX ADIABATIC CONNECTION
-We have recently shown that the complex scaled Fock operator Eq.~\eqref{eq:scaled_fock}
+We have recently shown that the complex scaled Fock operator \eqref{eq:scaled_fock}
 also allows states of different symmetries to be interconverted by following a well-defined
 contour in the complex $\lambda$-plane.\cite{Burton_2019}
 In particular, by slowly varying $\lambda$ in a similar (yet different) manner