+\scriptsize
+ \begin{minipage}[c]{0.1\textwidth}
+ \centering
+ \underline{G. Galilei}\\[0.1cm]
+ \includegraphics[width=0.93\textwidth]{galilei.eps}\\
+ {\tiny 1564--1642}\\[0.1cm]
+ \underline{H. Lorentz}\\[0.1cm]
+ \includegraphics[width=0.93\textwidth]{lorentz.eps}\\
+ {\tiny 1853--1928}\\[0.1cm]
+ \underline{A. Michelson}\\[0.1cm]
+ \includegraphics[width=0.93\textwidth]{michelson.eps}\\
+ {\tiny 1852--1931}\\[0.1cm]
+ \underline{E. Morley}\\[0.1cm]
+ \includegraphics[width=0.93\textwidth]{morley.eps}\\
+ {\tiny 1838--1923}
+ \end{minipage}
+ \begin{minipage}[c]{0.03\textwidth}
+ \hfill
+ \end{minipage}
+ \begin{minipage}[c]{0.85\textwidth}
+ \begin{minipage}{0.59\textwidth}
+ {\bf Galilei Transformation:}
+ $x'=x-vt\textrm{ , }\quad y'=y$
+ \begin{eqnarray}
+ F&=& m\frac{d^2}{dt^2}x'\nonumber\\
+ &=& m\frac{d^2}{dt^2}(x-vt)=
+ \frac{d}{dt}\left(\frac{d}{dt}x-v\right)=m\frac{d^2}{dt^2}x
+ \nonumber
+ \end{eqnarray}
+ \centering
+ Newton-Gleichungen ${\color{green}\surd}\quad$
+ Maxwell-Gleichungen ${\color{red}\times}$
+ \end{minipage}
+ \begin{minipage}{0.39\textwidth}
+ \begin{flushright}
+ \includegraphics[width=0.9\textwidth]{galileo.eps}
+ \end{flushright}
+ \end{minipage}\\[0.2cm]
+ \begin{minipage}{0.98\textwidth}
+ {\bf Lorentz Transformation} und {\bf Michelson Morley Interferometer}
+ \end{minipage}\\[0.2cm]
+ \begin{minipage}[t]{0.48\textwidth}
+ \includegraphics[width=0.9\textwidth]{interferometer.eps}
+ \end{minipage}
+ \begin{minipage}[t]{0.50\textwidth}
+ \includegraphics[width=0.95\textwidth]{mi_orig.eps}
+ \end{minipage}\\[0.3cm]
+ \begin{minipage}[t]{0.35\textwidth}
+ ${\color{red}t'_1}=\frac{L}{c-v}$,
+ ${\color{red}t'_2-t'_1}=\frac{L}{c+v}$\\
+ ${\color{red}t'_2}=\frac{2L}{c(1-v^2/c^2)}$\\[0.3cm]
+ $(c{\color{blue}t_1})^2=L^2+(v{\color{blue}t_1})^2$\\
+ ${\color{blue}t_1}=L/\sqrt{c^2-v^2}$\\
+ ${\color{blue}t_2}=\frac{2L}{c\sqrt{1-v^2/c^2}}$
+ \end{minipage}
+ \begin{minipage}[t]{0.63\textwidth}
+ Ergebnis: ${\color{red}t'_2}={\color{blue}t_2}$\\[0.2cm]
+ {\bf Lorentzkontraktion:} Bewegung relativ zum "Ather\\
+ $L\rightarrow L/\gamma\textrm {, }\quad\gamma=1/\sqrt{1-v^2/c^2}
+ \qquad\textrm{Maxwell-Gln} {\color{green}\surd}$\\[0.2cm]
+ {\bf Einstein --- spezielle Relativit"atstheorie}\\
+ Maxwell gilt in allen Inertialsystemen ($c=const.$)\\
+ Lorentz-Invarianz ${\color{green}\surd}\stackrel{v\rightarrow 0}{\rightarrow}$
+ Galilei-Invarianz ${\color{red}\times}$\\
+ Kein(e) absolute(r) Zeit/Raum mehr!
+ \end{minipage}
+ \end{minipage}
+\end{slide}
+
+\begin{slide}
+\footnotesize
+ \begin{minipage}[t]{0.11\textwidth}
+ \centering
+ \underline{M. Planck}\\[0.1cm]
+ \includegraphics[width=0.73\textwidth]{planck.eps}\\
+ {\tiny 1858--1947}\\[0.1cm]
+ \underline{A. Einstein}\\[0.1cm]
+ \includegraphics[width=0.73\textwidth]{einstein.eps}\\
+ {\tiny 1879--1955}\\[0.1cm]
+ \underline{de Broglie}\\[0.1cm]
+ \includegraphics[width=0.73\textwidth]{broglie.eps}\\
+ {\tiny 1892--1987}\\[0.1cm]
+ \underline{Schr"odinger}\\[0.1cm]
+ \includegraphics[width=0.73\textwidth]{schrodinger.eps}\\
+ {\tiny 1887--1961}
+ \end{minipage}
+ \begin{minipage}[t]{0.03\textwidth}
+ \hfill
+ \end{minipage}
+ \begin{minipage}[t]{0.84\textwidth}
+%
+ {\bf Quantenhypothese}\\[0.2cm]
+ "Ubertrag Energiemenge vom/zum Strahlungsfeld\\
+ $\Delta E=h\nu\textrm{, }\quad
+ h:\textrm{ Plancksches Wirkungsquantum}$\\[0.2cm]
+ $\rightarrow$ {\bf Plancksches Strahlungsgesetz}\\
+ Strahlungsverteilung des schwarzen K"orpers
+ \begin{picture}(0,0)(-26,30)
+ \includegraphics[width=4.0cm]{bb_dist.eps}
+ \end{picture}\\[0.3cm]
+%
+ {\bf Weiterf"uhrende Hypothese}\\[0.2cm]
+ Strahlungsfeld besteht aus Qaunten\\
+ Lichtuquanten haben Energie $E=h\nu$\\
+ $\rightarrow$ {\bf photoelektrischer Effekt}
+ \begin{picture}(0,0)(-27,5)
+ \includegraphics[width=2.5cm]{photo.eps}
+ \end{picture}\\
+ \begin{center}
+ \fbox{{\bf Welle-Teilchen-Dualismus}}\\
+ \end{center}
+ {\bf Postulat}\\
+ Masseteilchen mit Impuls haben Wellencharakter
+ und entsprechende Wellenl"ange\\
+ {\bf De Broglie Wellenl"ange} $\lambda=\frac{h}{p}$
+ \begin{picture}(0,0)(-10,80)
+ \includegraphics[width=6.5cm]{double_slit.eps}
+ \end{picture}\\[0.2cm]
+ {\bf Aufl"osung in der Quantenmechanik}
+ \begin{itemize}
+ \item Teilchen beschrieben durch\\
+ Wellenfunktion $\Psi(\vec{r},t)$
+ \item $|\Psi|^2\equiv$ Aufenthaltswahrscheinlichkeit
+ \item $\Psi(\vec{r},t)$ L"osungen\\
+ der Schr"odingergleichung
+ $i\hbar\frac{d}{dt}\Psi(\vec{r},t)=H\Psi(\vec{r},t)$
+ \end{itemize}
+ \end{minipage}