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\begin{document}
%INSIGHT SLIDE
\begin{slide}
  \centerline{\psframebox[fillstyle=solid,fillcolor=blue,framearc=.1,framesep=2mm]{\large\bfseries\color{yellow}Two Cases of Spectroscopic Modeling}}
\begin{multicols}{2}
\textbf{Plasmas formed during Laser Ablation}
  \begin{itemize}
     \item Most common laser produced plasma
     \item I$_{laser}=1\times10^{7}$ -- $1\times10^{10}$ W/cm$^2$
     \item T$_{e}$ = 1-3 eV 
     \item Stoichiometrically Complex targets 
     \item Time-dep. atomic kinetics ($N_{a}<10^{17} cm^{-3}$)
     \item Opacity and Lineshape effects become important ($N_{a}>10^{17} cm^{-3}$)
  \end{itemize}
\textbf{Intense Ultrashort Laser Plasmas}
  \begin{itemize}
     \item Far from equilibrium
     \item Non-Maxwellian free e$^{-}$ dis. func.
     \item Time-dep. atomic and e$^{-}$ kinetics
     \item I$_{laser}=1\times10^{15}$ -- $1\times10^{21}$ W/cm$^2$; $\tau=20-300 fs$
     \item T$_{e}$= 1000-1500 eV (Final T.E.)
     \item Ar cluster targets
  \end{itemize}
\end{multicols}
\end{slide}
\end{document}

