fix comments

main.tex

@@ -26,10 +26,12 @@
 \usepackage[usenames,dvipsnames]{xcolor}
 \usepackage{setspace}
 \usepackage[compact]{titlesec}
-%%%Please don't disable any packages in the preamble, as this may cause the template to display incorrectly.%%%
+%%% Please don't disable any packages in the preamble, as this may
+%%% cause the template to display incorrectly.%%%
 \usepackage{amsmath}
 
-\usepackage{epstopdf}%This line makes .eps figures into .pdf - please comment out if not required.
+\usepackage{epstopdf}%This line makes .eps figures into .pdf - please
+                     %comment out if not required.
 
 \definecolor{cream}{RGB}{222,217,201}
 
@@ -47,7 +49,8 @@
 }
 %%%END OF HEADER%%%
 
-%%%PAGE SETUP - Please do not change any commands within this section%%%
+%%%PAGE SETUP - Please do not change any commands within this
+%%% section%%%
 \makeFNbottom
 \makeatletter
 \renewcommand\LARGE{\@setfontsize\LARGE{15pt}{17}}
@@ -93,7 +96,8 @@
 \setlength\bibsep{1pt}
 %%%END OF FOOTER%%%
 
-%%%FIGURE SETUP - please do not change any commands within this section%%%
+%%%FIGURE SETUP - please do not change any commands within this
+%%% section%%%
 \makeatletter 
 \newlength{\figrulesep} 
 \setlength{\figrulesep}{0.5\textfloatsep} 
@@ -116,10 +120,8 @@
 \vspace{3cm}
 \sffamily
 \begin{tabular}{m{4.5cm} p{13.5cm} }
-
   \includegraphics{head_foot/DOI} & \noindent\LARGE{\textbf{ Plasma-Induced Symmetry Breaking in a Spherical Silicon Nanoparticle}} \\%Article title goes here instead of the text "This is the title"
   \vspace{0.3cm} & \vspace{0.3cm} \\
-
                                   & \noindent\large{Anton Rudenko,$^{\ast}$\textit{$^{a}$} Tatiana E. Itina,\textit{$^{a\ddag}$} Konstantin Ladutenko,\textit{$^{b}$} and Sergey Makarov\textit{$^{b}$}
  
                                     \textit{$^{a}$~Laboratoire Hubert Curien, UMR CNRS 5516, University of Lyon/UJM, 42000, Saint-Etienne, France }
@@ -128,7 +130,7 @@
                                     } \\%Author names go here instead of "Full name", etc.
  
  
-  \includegraphics{head_foot/dates} & \noindent\normalsize{The concept
+  \includegraphics{head_foot/dates} & \noindent\normalsize {The concept
 of nonlinear all-dielectric nanophotonics based on high refractive
 index (e.g., silicon) nanoparticles supporting magnetic optical
 response has recently emerged as a powerful tool for ultrafast
@@ -145,7 +147,7 @@ allows us to propose a novel concept of deeply subwavelength
 symmetrical silicon nanoparticle. More importantly, we reveal strong
 symmetry breaking in the initially symmetrical nanoparticle during
 ultrafast photoexcitation near the magnetic dipole resonance. The
-ultrafast manipulation by nanoparticle inherent structure and symmetry
+ultrafast manipulation by nanoparticle inherent structure and symmetry 
 paves the way to novel principles for nonlinear optical nanodevices.}
 
 \end{tabular}
@@ -166,21 +168,22 @@ F-42000, Saint-Etienne, France}} \footnotetext{\textit{$^{b}$~ITMO
 University, Kronverksiy pr. 49, St. Petersburg, Russia}}
 
 
-%Please use \dag to cite the ESI in the main text of the article.  %If
-you article does not have ESI please remove the the \dag symbol from
-the title and the footnotetext below.  \footnotetext{\dag~Electronic
-Supplementary Information (ESI) available: [details of any
-supplementary information available should be included here]. See DOI:
-10.1039/b000000x/} %additional addresses can be cited as above using
-the lower-case letters, c, d, e... If all authors are from the same
-address, no letter is required
+% Please use \dag to cite the ESI in the main text of the article.
 
-\footnotetext{\ddag~Additional footnotes to the title and authors can
-be included \emph{e.g.}\ `Present address:' or `These authors
-contributed equally to this work' as above using the symbols: \ddag,
-\textsection, and \P. Please place the appropriate symbol next to the
-author's name and include a \texttt{\textbackslash footnotetext} entry
-in the the correct place in the list.}
+% If you article does not have ESI please remove the the \dag symbol
+% from the title and the footnotetext below.
+% \footnotetext{\dag~Electronic Supplementary Information (ESI)
+% available: [details of any supplementary information available
+% should be included here]. See DOI:10.1039/b000000x/} %additional
+% addresses can be cited as above using the lower-case letters, c, d,
+% e... If all authors are from the same address, no letter is required
+
+% \footnotetext{\ddag~Additional footnotes to the title and authors can
+% be included \emph{e.g.}\ `Present address:' or `These authors
+% contributed equally to this work' as above using the symbols: \ddag,
+% \textsection, and \P. Please place the appropriate symbol next to the
+% author's name and include a \texttt{\textbackslash footnotetext} entry
+% in the the correct place in the list.}
 
 
 %%%END OF FOOTNOTES%%%
@@ -248,29 +251,27 @@ optical nanoantennas.
 %\begin{itemize}
 %\item Fig.1: Beautiful conceptual picture
 %\item Fig.2: Temporal evolution of EHP in NP with different diameters
-at fixed intensity, in order to show that we have the highest
-asymmetry around magnetic dipole (MD) resonance. This would be really
-nice!
+%at fixed intensity, in order to show that we have the highest
+%asymmetry around magnetic dipole (MD) resonance. This would be really
+%nice!
 %\item Fig.3: Temporal evolution of EHP in NP with fixed diameter (at
-MD) at different intensities, in order to show possible regimes of
-plasma-patterning of NP volume. It would be nice, if we will show
-power patterns decencies on intensity for side probe pulse to show
-beam steering due to symmetry breaking.
+%MD) at different intensities, in order to show possible regimes of
+%plasma-patterning of NP volume. It would be nice, if we will show
+%power patterns decencies on intensity for side probe pulse to show beam steering due to symmetry breaking.
 %\item Fig.4: (a) Dependence on pulse duration is also interesting. We
-have to show at which duration the asymmetry factor is saturated. (b)
-2D map of asymmetry factor in false colors, where x-axis and y-axis
-correspond to intensity and NP diameter.
+%have to show at which duration the asymmetry factor is saturated. (b)
+%2D map of asymmetry factor in false colors, where x-axis and y-axis correspond to intensity and NP diameter.
 %\end{itemize} %Additionally, if you will manage to calculate
-evolution of scattering power pattern and show considerable effect of
-beam steering, we can try Nanoscale or LPR, because the novelty will
-be very high.
+%evolution of scattering power pattern and show considerable effect of
+% beam steering, we can try Nanoscale or LPR, because the novelty will
+% be very high.
 
 
- \section{Modeling details}
+\section{Modeling details}
  
- %TEI for Anton: please describe what you model first (what physical
-processes). Then, we speak about "pulse", but never "laser". Should we
-provide more details concerning irradiation source?
+% TEI for Anton: please describe what you model first (what physical
+% processes). Then, we speak about "pulse", but never "laser". Should
+% we provide more details concerning irradiation source?
 
 We focus out attention on silicon because this material is promising
 for the implementation of nonlinear photonic devices thanks to a broad
@@ -308,24 +309,24 @@ permittivity of non-excited silicon at $800$ nm wavelength [green1995]
 includes the contribution due to heating of the conduction band,
 described by the differential equation derived from the Drude model
 \begin{equation} \label{Drude}
-\displaystyle{\frac{\partial{\vec{J}}}{\partial{t}} = - \nu_e\vec{J} +
-\frac{e^2n_e(t)}{m_e^*}\vec{E}}, \end{equation} where $e$ is the
+  \displaystyle{\frac{\partial{\vec{J}}}{\partial{t}} = - \nu_e\vec{J}
+    + \frac{e^2n_e(t)}{m_e^*}\vec{E}}, \end{equation} where $e$ is the
 elementary charge, $m_e^* = 0.18m_e$ is the reduced electron-hole mass
 [sokolowski2000]\cite{Sokolowski2000}, $n_e(t)$ is the time-dependent
 free carrier density and $\nu_e = 10^{15} s^{-1}$ is the electron
 collision frequency [sokolowski2000]\cite{Sokolowski2000}. Silicon
 nanoparticle is surrounded by air, where the light propagation is
-calculated by Maxwell's equations with $\vec{J} = 0$ and $\epsilon =
-1$. The system of Maxwell's equations coupled with electron density
-equations is solved by the finite-difference numerical method
-[rudenko2016]%\cite{Rudenko2016} , based on the finite-difference
-time-domain (FDTD) method [yee1966] \cite{Yee1966} and
-auxiliary-differential method for disperse media
+calculated by Maxwell's equations with $\vec{J} = 0$ and
+$\epsilon = 1$. The system of Maxwell's equations coupled with
+electron density equations is solved by the finite-difference
+numerical method [rudenko2016]\cite{Rudenko2016} , based on the
+finite-difference time-domain (FDTD) method [yee1966] \cite{Yee1966}
+and auxiliary-differential method for disperse media
 [taflove1995]\cite{Taflove1995}. At the edges of the grid, we apply
 absorbing boundary conditions related to convolutional perfect matched
-layers (CPML) to avoid nonphysical reflections [roden2000]%
-\cite{Roden2000} . Initial electric field is introduced as a Gaussian
-focused beam source as follows
+layers (CPML) to avoid nonphysical reflections
+[roden2000]\cite{Roden2000} . Initial electric field is introduced as
+a Gaussian focused beam source as follows
 \begin{align}
 \begin{aligned}
 \label{Gaussian} {E_x}(t, r, z) =
@@ -532,8 +533,8 @@ with electron plasma inside.}
 %\begin{figure} %\centering
 % \includegraphics[height=0.7\linewidth]{Si-flow-R140-XYZ-Eabs}
 % \caption{EHP distributions for nonres., MD, ED, and MQ nanoparticles
-at moderate photoexcitation. The aim is to show different possible EHP
-patterns and how strong could be symmetry breaking.
+% at moderate photoexcitation. The aim is to show different possible
+% EHP patterns and how strong could be symmetry breaking.
 % \label{fgr:example}
 %\end{figure}
 
@@ -593,19 +594,21 @@ have found describing experiments and previous calculations
 
 
 %The \balance command can be used to balance the columns on the final
-page if desired. It should be placed anywhere within the first column
-of the last page.
+%page if desired. It should be placed anywhere within the first column
+%of the last page.
 
 %\balance
 
 %If notes are included in your references you can change the title
-from 'References' to 'Notes and references' using the following
-command: %\renewcommand\refname{Notes and references}
+% from 'References' to 'Notes and references' using the following
+% command:
+
+% \renewcommand\refname{Notes and references}
 
 %%%REFERENCES%%%
 
 \bibliography{References.bib} %You need to replace "rsc" on this line
-with the name of your .bib file \bibliographystyle{rsc} %the RSC's
-.bst file
+                              %with the name of your .bib file
+\bibliographystyle{rsc} %the RSC's .bst file
 
 \end{document}