diff --git a/Manuscript/EPAWTFT.tex b/Manuscript/EPAWTFT.tex
index 47e7b5a..33fa43c 100644
--- a/Manuscript/EPAWTFT.tex
+++ b/Manuscript/EPAWTFT.tex
@@ -1175,7 +1175,7 @@ where we consider one of the sites as a ``ghost atom'' that acts as a
 destination for ionised electrons being originally localised on the other site.
 To mathematically model this scenario in this asymmetric Hubbard dimer, we introduce a one-electron potential $-\epsilon$ on the left site to 
 represent the attraction between the electrons and the model ``atomic'' nucleus [see Eq.~\eqref{eq:H_FCI}], where we define $\epsilon > 0$.
-The reference Slater determinant for a doubly-occupied atom can be represented using the RHF
+The reference Slater determinant for a doubly-occupied atom can be represented using RHF
 orbitals [see Eq.~\eqref{eq:RHF_orbs}] with $\theta_{\alpha}^{\text{RHF}} = \theta_{\beta}^{\text{RHF}} = 0$, 
 which corresponds to strictly localising the two electrons on the left site.
 %and energy