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| -rw-r--r-- | buch/papers/parzyl/img/D_plot.png | bin | 0 -> 712446 bytes | |||
| -rw-r--r-- | buch/papers/parzyl/img/v_plot.png | bin | 0 -> 637451 bytes | |||
| -rw-r--r-- | buch/papers/parzyl/teil1.tex | 16 |
3 files changed, 14 insertions, 2 deletions
diff --git a/buch/papers/parzyl/img/D_plot.png b/buch/papers/parzyl/img/D_plot.png Binary files differnew file mode 100644 index 0000000..f76e35b --- /dev/null +++ b/buch/papers/parzyl/img/D_plot.png diff --git a/buch/papers/parzyl/img/v_plot.png b/buch/papers/parzyl/img/v_plot.png Binary files differnew file mode 100644 index 0000000..b8c803e --- /dev/null +++ b/buch/papers/parzyl/img/v_plot.png diff --git a/buch/papers/parzyl/teil1.tex b/buch/papers/parzyl/teil1.tex index a56d94b..673fa7f 100644 --- a/buch/papers/parzyl/teil1.tex +++ b/buch/papers/parzyl/teil1.tex @@ -88,7 +88,7 @@ Whittaker und Watson zeigen in \cite{parzyl:whittaker} eine Lösung M_{\frac{1}{2} n + \frac{1}{4}, - \frac{1}{4}} \left(\frac{1}{2}z^2\right) + \frac{ - \Gamma\left(-{\textstyle \frac{1}{2}}\right) 2^{\frac{1}{2}n + \frac{1}{2}} z^{-\frac{1}{2}} + \Gamma\left(-{\textstyle \frac{1}{2}}\right) 2^{\frac{1}{2}n + \frac{1}{4}} z^{-\frac{1}{2}} }{ \Gamma\left(- {\textstyle \frac{1}{2}} n\right) } @@ -132,4 +132,16 @@ ausgedrückt werden V(a,z) &= \frac{\Gamma \left({\textstyle \frac{1}{2}} + a\right)}{\pi} \left[\sin\left(\pi a\right) D_{-a-1/2}(z) + D_{-a-1/2}(-x)\right]. \end{align} -TODO Plot
\ No newline at end of file +TODO Plot +\begin{figure} + \centering + \includegraphics[scale=0.3]{papers/parzyl/img/D_plot.png} + \caption{$D_a(z)$ mit unterschiedlichen Werten für $a$.} + \label{parzyl:fig:dnz} +\end{figure} +\begin{figure} + \centering + \includegraphics[scale=0.3]{papers/parzyl/img/v_plot.png} + \caption{$V(a,z)$ mit unterschiedlichen Werten für $a$.} + \label{parzyl:fig:Vnz} +\end{figure}
\ No newline at end of file |
