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-\includegraphics{head_foot/DOI} & \noindent\LARGE{\textbf{This is the title$^\dag$}} \\%Article title goes here instead of the text "This is the title"
+\includegraphics{head_foot/DOI} & \noindent\LARGE{\textbf{ Plasma-induced breaking symmetry by ultrafast laser irradiation of $\pmb{Si}$ nanoparticle }} \\%Article title goes here instead of the text "This is the title"
 \vspace{0.3cm} & \vspace{0.3cm} \\
 
- & \noindent\large{Full Name,$^{\ast}$\textit{$^{a}$} Full Name,\textit{$^{b\ddag}$} and Full Name\textit{$^{a}$}} \\%Author names go here instead of "Full name", etc.
+ & \noindent\large{Anton Rudenko,$^{\ast}$\textit{$^{a}$} Tatiana Itina,\textit{$^{b\ddag}$} Konstantin Ladutenko,\textit{$^{a}$} and Sergey Makarov\textit{$^{a}$}} \\%Author names go here instead of "Full name", etc.
 
 \includegraphics{head_foot/dates} & \noindent\normalsize{The abstract should be a single paragraph which summarises the content of the article. Any references in the abstract should be written out in full \textit{e.g.} [Surname \textit{et al., Journal Title}, 2000, \textbf{35}, 3523].} \\%The abstract goes here instead of the text "The abstract should be..."
 
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+ I would say that switching of scattering properties was conceptually studied in our recent works.
+ 
+1)      A single nanoparticle for tuning of front-to-back ratio: http://pubs.acs.org/doi/abs/10.1021/acs.nanolett.5b02534 ; http://pubs.acs.org/doi/abs/10.1021/acsphotonics.6b00358
+
+2)      A dimer for beam steering: https://arxiv.org/abs/1606.05199 (accepted in Las.Phot.Rev.)
+
+ 
+All these studies were carried out analytically assuming homogenized dielectric permittivity.
+ 
+Next step is to show numerically how EHP is distributed in a nanoparticle with temporal evolution. The most interesting result is the plasma-induced breaking symmetry which potentially might be useful for beam steering or enhanced second harmonics generation. I believe, there is enough novelty to publish such results at least in ACS Photonics. For instance, we can show temporal EHP evolution at different intensities, NP diameters and durations. Finally, we can introduce some parameter of the nanoparticle asymmetry (ratio of EHP density in front and back sides of NP), which can be represented as a 2D map.
+ 
+I suggest such plan:
+
+\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!
+\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.
+\item Fig.4: Dependence on pulse duration is also interesting. We have to show at which durations the asymmetry factor is saturated.
+\item Fig.5: 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.
+ 
+I have discuss this concept with a number of my colleagues, including Yuri Kivshar. Honestly, all of them said that such work could be interesting, because no one studied EHP distribution inside a Si nanoparticle.
+
 The main text of the article\cite{Mena2000} should appear here.
 
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 \begin{figure}[h]
 \centering
-  \includegraphics[height=3cm]{example}
+  \includegraphics[height=0.7\linewidth]{Si-flow-R140-XYZ-Eabs}
   \caption{An example figure caption}
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