ab nach nepal! :)

diff --git a/nlsop/nlsop_emrs_2004.tex b/nlsop/nlsop_emrs_2004.tex
index 221b6a8a482da199c8ec4a774eb863c2e0eaee08..fa65407458216dcfd649cefdadeae5808e632600 100644 (file)
--- a/nlsop/nlsop_emrs_2004.tex
+++ b/nlsop/nlsop_emrs_2004.tex
@@ -93,7 +93,17 @@ Finally a standard diffusion algorithm is started, so the supersaturation of car
 \newpage
 
 \section{Results}
+Figure \ref{4} shows a comparison of a simulation result and a cross-sectional TEM snapshot of $180 \, keV$ implanted carbon in silicon at $150 \,^{\circ} \mathrm{C}$ with $4.3 \times 10^{17} cm^{-2}$. The depth the lamella structure is starting in ($300 \, nm$) and also the average length of these precipitates complies to that one of the experimental data. The arrays are ordered in uniform intervals. It can be seen that lamella selforganized structures can be reproduced by the simulation.
 
+Furthermore conditions for observing lamella structures can be specified. Figure \ref{5} shows two identical simulation cycles with diffusion in $z$-direction switched off and on. The lamella structures only appear when diffusion in $z$-direction \ldots
+
+TODO:\\
+- diffusion rate -> depth of lamella structures\\
+- complementary arrays of c/a precipitates for z and z+1\\
+- evt FFT bilder\\
+- summary\\
+
+\newpage
 
 \section{Conclusion}
 
@@ -131,4 +141,18 @@ Finally a standard diffusion algorithm is started, so the supersaturation of car
 \end{center}
 \end{figure}
 
+\begin{figure}[!h]
+\begin{center}
+\includegraphics[width=15cm]{if_cmp2_e.eps}
+\caption[Comparison of a simulation result and a cross-sectional TEM snapshot of $180 \, keV$ implanted carbon in silicon at $150 \,^{\circ} \mathrm{C}$ with $4.3 \times 10^{17} cm^{-2}$]{} \label{4}
+\end{center}
+\end{figure}
+
+\begin{figure}[!h]
+\begin{center}
+\includegraphics[width=15cm]{mit_ohne_diff.eps}
+\caption[Identical simulation cycles, with diffusion switched off (left) and on (right)]{} \label{5}
+\end{center}
+\end{figure}
+
 \end{document}