@@ -3585,7 +3585,7 @@ \subsubsection{Generation of the silica block}
35853585run 30000
35863586\end {lstlisting }
35873587{\color {blue} In this case, the initial and final target temperatures
3588- set for the Nose -Hoover thermostat is different, causing it to evolve
3588+ set for the Nos \' e -Hoover thermostat is different, causing it to evolve
35893589linearly within the number of timesteps evoked in the \lmpcmd {run}
35903590command. }
35913591In the third step, the system is equilibrated at the final desired
@@ -3695,7 +3695,6 @@ \subsubsection{Adding water}
36953695
36963696% \paragraph{Using hydrid potentials}
36973697
3698- {\color {blue}
36993698\paragraph {Adapting the pair style }
37003699
37013700% The first {\color{blue}peculiarity} of our system is that it combines water and
@@ -3725,11 +3724,11 @@ \subsubsection{Adding water}
37253724\end {lstlisting }
37263725% Combining the two force fields, Vashishta and TIP4P/2005, is achieved
37273726% using the \lmpcmd{hybrid/overlay} pair style.
3728- The PPPM solver~\cite {luty1996calculating } is specified with the \lmpcmd {kspace}
3727+ { \color {blue} The PPPM solver~\cite {luty1996calculating } is specified with the \lmpcmd {kspace}
37293728command, and is used to compute the long-range Coulomb interactions associated
37303729with \lmpcmd {tip4p/long}. Finally, the {\color {blue} form of} the bond
3731- and angle{ \color {blue} potentials} of the water molecules are defined; however,
3732- { \color {blue} as previously discussed,} these specifications are
3730+ and angle potentials of the water molecules are defined; however,
3731+ as previously discussed, these specifications are
37333732not critical since TIP4P/2005 is a rigid water model.}
37343733
37353734\begin {note }
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