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@@ -508,7 +508,7 @@ license.
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radii $R = 75$ nm (a-d), $R = 100$ nm (e-h) and $R = 115$ nm (i-l)
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radii $R = 75$ nm (a-d), $R = 100$ nm (e-h) and $R = 115$ nm (i-l)
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taken at different times and conditions of excitation (stages
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taken at different times and conditions of excitation (stages
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$1-4$: (1) first optical cycle, (2) extremum at few optical cycles,
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$1-4$: (1) first optical cycle, (2) extremum at few optical cycles,
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- (3) Mie theory, (4) nonlinear effects). Pulse duration $50\:f\!s$
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+ (3) Mie theory, (4) nonlinear effects). Pulse duration $50$~\textit{fs}
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(FWHM). Wavelength $800$ nm in air. Peak laser fluence is fixed to
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(FWHM). Wavelength $800$ nm in air. Peak laser fluence is fixed to
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be $0.125$ J/cm$^2$.}
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be $0.125$ J/cm$^2$.}
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\end{figure*}
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\end{figure*}
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@@ -520,7 +520,7 @@ license.
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of the average EHP density in the front part of the nanoparticle
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of the average EHP density in the front part of the nanoparticle
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(a, c, e) and time (b, d, f) for different Si nanoparticle radii
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(a, c, e) and time (b, d, f) for different Si nanoparticle radii
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(a, b) $R = 75$ nm, (c, d) $R = 100$ nm, (e, f) $R = 115$ nm. Pulse
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(a, b) $R = 75$ nm, (c, d) $R = 100$ nm, (e, f) $R = 115$ nm. Pulse
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- duration $50\:f\!s$ (FWHM). Wavelength $800$ nm in air. (a, c, e)
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+ duration $50$~\textit{fs} (FWHM). Wavelength $800$ nm in air. (a, c, e)
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Different stages of EHP evolution shown in \ref{fig2} are
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Different stages of EHP evolution shown in \ref{fig2} are
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indicated. (b, d, f) The temporal evolution of Gaussian beam
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indicated. (b, d, f) The temporal evolution of Gaussian beam
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intensity is also shown. Peak laser fluence is fixed to be $0.125$
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intensity is also shown. Peak laser fluence is fixed to be $0.125$
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