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@@ -21,6 +21,7 @@
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\usepackage{float}
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\usepackage{fancyhdr}
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\usepackage{fnpos}
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+\usepackage{tabularx}
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\usepackage[english]{babel}
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\usepackage{array}
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\usepackage{droidsans}
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@@ -327,9 +328,13 @@ where $I=\frac{n}{2}\sqrt{\frac{\epsilon_0}{\mu_0}}\left|\vec{E}\right|^2$ is th
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\begin{figure*}[ht!]
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\centering
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+\begin{tabular*}{0.73\textwidth}{ c@{\extracolsep{\fill}} c@{\extracolsep{\fill}} c@{\extracolsep{\fill}} c@{\extracolsep{\fill}} c}
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+$-80 fs$&$-60 fs$&$-30 fs$&$ -20 fs$&$ -10 fs$\\
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+\end{tabular*}
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\includegraphics[width=0.9\textwidth]{2nm_75}
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+\includegraphics[width=0.9\textwidth]{2nm_100}
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\includegraphics[width=0.9\textwidth]{2nm_115}
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-\caption{\label{plasma-105nm} Split figure \ref{fig2} into two, this is first part.}
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+\caption{\label{plasma-105nm} Pulse duration 80~fs Split figure \ref{fig2} into two, this is first part.}
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\end{figure*}
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The changes of the real and imaginary parts of the permittivity associated with the time-dependent free carrier response \cite{Sokolowski2000} can be derived from equations (\ref{Maxwell}, \ref{Drude}) and are written as follows
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