diff --git a/Manuscript/FarDFT.tex b/Manuscript/FarDFT.tex
index c1292eb..5fbb85c 100644
--- a/Manuscript/FarDFT.tex
+++ b/Manuscript/FarDFT.tex
@@ -471,20 +471,13 @@ For all calculations, we use the aug-cc-pVXZ (X = D, T, Q, and 5) Dunning family
 Numerical quadratures are performed with the \texttt{numgrid} library \cite{numgrid} using 194 angular points (Lebedev grid) and a radial precision of $10^{-6}$. \cite{Becke_1988b,Lindh_2001}
 This study deals only with spin-unpolarised systems, \ie, $\n{\uparrow}{} = \n{\downarrow}{} = \n{}{}/2$ (where $\n{\uparrow}{}$ and $\n{\downarrow}{}$ are the spin-up and spin-down electron densities).
 Moreover, we restrict our study to the case of a two-state ensemble (\ie, $\nEns = 2$) where both the ground state ($I=0$ with weight $1 - \ew{}$) and the first doubly-excited state ($I=1$ with weight $\ew{}$) are considered. 
-Although one should have $0 \le \ew{} \le 1/2$ to ensure the GOK variational principle, we will sometimes ``violate'' this variational constraint.
+\titou{To ensure the GOK variational principle, one should then have $0 \le \ew{} \le 1/2$. 
+However, we will sometimes ``violate'' this variational constraint.
 Indeed, the limit $\ew{} = 1$ is of particular interest as it corresponds to a genuine saddle point of the KS equations, and match perfectly the results obtained with the maximum overlap method (MOM) developed by Gilbert, Gill and coworkers. \cite{Gilbert_2008,Barca_2018a,Barca_2018b}
-\manu{I think we need to be a bit more clear about the $\ew{} = 1$ case, as
-it stands a little bit beyond the theory discussed previously. What you
-are looking at in the range $1/2\leq \ew{}\leq 1$ are, indeed, other
-stationary points (than the minimizing ones) of the density matrix
-operator functional in Eq.~\eqref{eq:min_KS_DM}. I would say that we
-look at these solutions for analysis purposes. I personally never looked
-(formally) at these solutions and their physical meaning. One should clearly
-mention that applying GOK-DFT in this range of weights would simply
-consists in switching ground and first excited states if a true
-minimization of the ensemble energy were performed. From this point of
-view we do not violate anything. 
-} 
+Although the range $1/2 < \ew{} \leq 1$ stands a little bit beyond the theory discussed previously, we look at these solutions for analysis purposes mainly.
+These solutions of the density matrix operator functional in Eq.~\eqref{eq:min_KS_DM} correspond to stationary points rather than minimising ones.
+Applying GOK-DFT in this range of weights would simply consists in switching the ground and excited states if true minimisations of the ensemble energy were performed.}
+
 
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \section{Results}