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[vorlesung] II.2 Formatierung für Randbemerkung nun zweizeilig

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Oliver Groß 2008-06-30 15:05:44 +02:00
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kapII-2.tex
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@ -121,7 +121,7 @@ Heisenberg:
für Gauss'sches Wellenpacket ist Gleichheit erreicht. für Gauss'sches Wellenpacket ist Gleichheit erreicht.
\paragraph*{Dynamik} \paragraph*{Dynamik}
\begin{align} \begin{align}
\psi(x,t) &= \intgr{-\infty}{+infty}{U(x,t; x',t_0)}{x'} &\left| t_0 = 0; ~ U(x,t; x',t_0) = \dirac{x}{U(t,t_0}{x'} \right.\\ \psi(x,t) &= \intgr{-\infty}{+infty}{U(x,t; x',t_0)}{x'} &\left| \begin{array}{l} t_0 = 0;\\ U(x,t; x',t_0) = \dirac{x}{U(t,t_0}{x'} \end{array} \right.\\
&= \left( \sqrt{\pi} \left( \Delta + \frac{i \hbar t}{m \Delta} \right) \right)^{-\frac{1}{2}} e^\frac{-\left(x - \frac{p_0 t}{m} \right)^2}{2 \Delta^2 \left( 1 + i \hbar \frac{t}{m \Delta^2} \right)} e^{\frac{i p_0}{\hbar} \left( x - \frac{p_0 t}{m} \right)} &= \left( \sqrt{\pi} \left( \Delta + \frac{i \hbar t}{m \Delta} \right) \right)^{-\frac{1}{2}} e^\frac{-\left(x - \frac{p_0 t}{m} \right)^2}{2 \Delta^2 \left( 1 + i \hbar \frac{t}{m \Delta^2} \right)} e^{\frac{i p_0}{\hbar} \left( x - \frac{p_0 t}{m} \right)}
\end{align} \end{align}
\begin{equation} \begin{equation}