|
|
@@ -299,8 +299,8 @@ the high melting temperature ($\approx 1690$~K), whereas its nonlinear
|
|
|
optical properties were extensively studied during the last
|
|
|
decades~\cite{Van1987, Sokolowski2000, leuthold2010nonlinear}. High
|
|
|
silicon melting point typically preserves structures formed from this
|
|
|
-material up to the EHP densities on the order of the critical value
|
|
|
-$N_{cr} \approx 5\cdot{10}^{21}$~cm$^{-3}$ \cite{Korfiatis2007}. At
|
|
|
+material up to the EHP densities on the order of the critical value~\cite{Korfiatis2007}
|
|
|
+$N_{cr} \approx 5\cdot{10}^{21}$~cm$^{-3}$. At
|
|
|
the critical density and above, silicon acquires metallic properties
|
|
|
($Re(\epsilon) < 0$) and contributes to the EHP reconfiguration during
|
|
|
ultrashort laser irradiation.
|
|
|
@@ -466,7 +466,7 @@ GitHub~\cite{Scattnlay-web} under open source license.
|
|
|
|
|
|
\begin{figure*}[p]
|
|
|
\centering
|
|
|
- \includegraphics[width=145mm]{time-evolution-I-no-NP.pdf}
|
|
|
+ \includegraphics[width=140mm]{time-evolution-I-no-NP.pdf}
|
|
|
\caption{\label{time-evolution} Temporal EHP (a, c, e) and asymmetry
|
|
|
factor $G_{N_e}$ (b, d, f) evolution for different Si nanoparticle
|
|
|
radii of (a, b) $R = 75$~nm, (c, d) $R = 100$~nm, and (e, f)
|
|
|
@@ -483,7 +483,7 @@ GitHub~\cite{Scattnlay-web} under open source license.
|
|
|
|
|
|
\begin{figure*}
|
|
|
\centering
|
|
|
- \includegraphics[width=150mm]{plasma-grid.pdf}
|
|
|
+ \includegraphics[width=145mm]{plasma-grid.pdf}
|
|
|
\caption{\label{plasma-grid} EHP density snapshots inside Si
|
|
|
nanoparticle of radii $R = 75$~nm (a-d), $R = 100$~nm (e-h) and
|
|
|
$R = 115$~nm (i-l) taken at different times and conditions of
|
|
|
@@ -620,7 +620,7 @@ GitHub~\cite{Scattnlay-web} under open source license.
|
|
|
resonant size for $R = 115$~nm the $G_{N_e} < 0$ due to the fact that
|
|
|
EHP is dominantly localized in the back side of the NP.
|
|
|
|
|
|
- In other words, due to a quasi-stationary pumping during Stage~3,
|
|
|
+ Due to a quasi-stationary pumping during Stage~3,
|
|
|
it is superposed with Stage~1 field pattern, resulting in an
|
|
|
additional EHP localized in the front side. This can be seen when
|
|
|
comparing result from the Mie theory in Fig.~\ref{mie-fdtd}(d) with
|
