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Tabellenanhang - Alex-weingarten.de

Tabellenanhang - Alex-weingarten.de

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O.3. FORMELN IM QUELLTEXT 87<br />

\begin{equation}<br />

\prod_{j\ge0}\left( \sum_{k\ge0} a_{jk}z^k \right) =<br />

\sum_{n \ge0} z^n \left(\sum_{h_0,k_1\ldots\ge0<br />

\atop k_0+k_1+\cdots=0}<br />

a_{0k_o} a_{1k_1}\ldots \right)<br />

\end{equation}<br />

\begin{equation}<br />

\vec x =<br />

\left( \begin{array}{c}<br />

x - x_s \\<br />

y - y_s \\<br />

z - z_s \\<br />

\end{array} \right)<br />

\end{equation}<br />

\begin{minipage}{120mm}<br />

\begin{displaymath}<br />

{\bf\Psi} = \left( \begin{array}{cc}<br />

\displaystyle{ab \choose cd}<br />

& \displaystyle \frac{e+f}{g-h} \\<br />

\Re z & \displaystyle \left| {ij \atop kl} \right|<br />

\end{array} \right)<br />

\end{displaymath}<br />

\end{minipage}<br />

\stepcounter{equation}<br />

\hspace*{\fill} (\theequation)\makebox[0pt][l]{\footnotemark}<br />

\footnotetext{Fette Griechen gibt es nur als Gro\3buchstaben.<br />

Die Erzeugung dieser Fu\3note war "ubrigens nicht einfach.}<br />

\vspace{1mm}<br />

\begin{equation}<br />

dE_\omega = V \frac{\hbar}{\pi^2 c^3}\omega^3 \cdot<br />

e ^{-\frac{\hbar \omega} {T}} \cdot d\omega<br />

\end{equation}<br />

\begin{equation}<br />

\oint \vec E\:d\vec s = - \frac {\,\partial}{\partial t}<br />

\int \vec B \:d\vec A<br />

\end{equation}<br />

\begin{equation}<br />

\frac{1}{2 \pi j} \int\limits_{x-j\infty}^{x+j\infty}<br />

e^{ts} \:f(s)\:ds =<br />

\left\{\begin{array}{r@{\quad \mbox{f"ur} \quad}l}<br />

0 & t < 0\\<br />

F(t) & t > 0

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