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Diffstat (limited to 'buch/papers/zeta')
30 files changed, 9592 insertions, 227 deletions
diff --git a/buch/papers/zeta/analytic_continuation.tex b/buch/papers/zeta/analytic_continuation.tex index 0ccc116..d45a6ae 100644 --- a/buch/papers/zeta/analytic_continuation.tex +++ b/buch/papers/zeta/analytic_continuation.tex @@ -3,16 +3,16 @@ Die analytische Fortsetzung der Riemannschen Zetafunktion ist äusserst interessant. Sie ermöglicht die Berechnung von $\zeta(-1)$ und weiterer spannender Werte. -So liegen zum Beispiel unendlich viele Nullstellen der Zetafunktion bei $\Re(s) = 0.5$. -Diese sind relevant für die Primzahlverteilung und sind Gegenstand der Riemannschen Vermutung. +So liegen zum Beispiel unendlich viele Nullstellen der Zetafunktion bei $\Re(s) = \frac{1}{2}$. +Wie bereits erwähnt sind diese Gegenstand der Riemannschen Vermutung. Es werden zwei verschiedene Fortsetzungen benötigt. Die erste erweitert die Zetafunktion auf $\Re(s) > 0$. -Die zweite verwendet eine Spiegelung an der $\Re(s) = 0.5$ Linie und erschliesst damit die ganze komplexe Ebene. +Die zweite verwendet eine Spiegelung an der $\Re(s) = \frac{1}{2}$ Geraden und erschliesst damit die ganze komplexe Ebene. Eine grafische Darstellung dieses Plans ist in Abbildung \ref{zeta:fig:continuation_overview} zu sehen. \begin{figure} \centering - \input{papers/zeta/continuation_overview.tikz.tex} + \input{papers/zeta/images/continuation_overview.tikz.tex} \caption{ Die verschiedenen Abschnitte der Riemannschen Zetafunktion. Die originale Definition von \eqref{zeta:equation1} ist im grünen Bereich gültig. @@ -23,7 +23,7 @@ Eine grafische Darstellung dieses Plans ist in Abbildung \ref{zeta:fig:continuat \end{figure} \subsection{Fortsetzung auf $\Re(s) > 0$} \label{zeta:subsection:auf_bereich_ge_0} -Zuerst definieren die Dirichletsche Etafunktion als +Zuerst definieren wir die Dirichletsche Etafunktion als \begin{equation}\label{zeta:equation:eta} \eta(s) = @@ -36,26 +36,40 @@ Diese Etafunktion konvergiert gemäss dem Leibnitz-Kriterium im Bereich $\Re(s) Wenn wir es nun schaffen, die sehr ähnliche Zetafunktion durch die Etafunktion auszudrücken, dann haben die gesuchte Fortsetzung. Zuerst wiederholen wir zweimal die Definition der Zetafunktion \eqref{zeta:equation1}, wobei wir sie einmal durch $2^{s-1}$ teilen \begin{align} - \zeta(s) + \color{red} + \zeta(s) &= \sum_{n=1}^{\infty} - \frac{1}{n^s} \label{zeta:align1} + \color{red} + \frac{1}{n^s} \label{zeta:align1} \\ - \frac{1}{2^{s-1}} - \zeta(s) + \color{blue} + \frac{1}{2^{s-1}} + \zeta(s) &= \sum_{n=1}^{\infty} - \frac{2}{(2n)^s}. \label{zeta:align2} + \color{blue} + \frac{2}{(2n)^s}. \label{zeta:align2} \end{align} Durch Subtraktion der beiden Gleichungen \eqref{zeta:align1} minus \eqref{zeta:align2}, ergibt sich \begin{align} - \left(1 - \frac{1}{2^{s-1}} \right) + \left({\color{red}1} - {\color{blue}\frac{1}{2^{s-1}}} \right) \zeta(s) &= - \frac{1}{1^s} - \underbrace{-\frac{2}{2^s} + \frac{1}{2^s}}_{-\frac{1}{2^s}} - + \frac{1}{3^s} - \underbrace{-\frac{2}{4^s} + \frac{1}{4^s}}_{-\frac{1}{4^s}} + {\color{red}\frac{1}{1^s}} + \underbrace{ + - + {\color{blue}\frac{2}{2^s}} + + + {\color{red}\frac{1}{2^s}} + }_{\displaystyle{-\frac{1}{2^s}}} + + + {\color{red}\frac{1}{3^s}} + \underbrace{- + {\color{blue}\frac{2}{4^s}} + + + {\color{red}\frac{1}{4^s}} + }_{\displaystyle{-\frac{1}{4^s}}} \ldots \\ &= \eta(s). @@ -75,7 +89,7 @@ Wir beginnen damit, die Gammafunktion für den halben Funktionswert zu berechnen = \int_0^{\infty} t^{\frac{s}{2}-1} e^{-t} dt. \end{equation} -Nun substituieren wir $t$ mit $t = \pi n^2 x$ und $dt=\pi n^2 dx$ und erhalten +Nun substituieren wir $t = \pi n^2 x$ und $dt=\pi n^2 dx$ und erhalten \begin{equation} \Gamma \left( \frac{s}{2} \right) = @@ -87,86 +101,33 @@ Nun substituieren wir $t$ mit $t = \pi n^2 x$ und $dt=\pi n^2 dx$ und erhalten \end{equation} Analog zum Abschnitt \ref{zeta:section:zusammenhang_mit_gammafunktion} teilen wir durch $(\pi n^2)^{\frac{s}{2}}$ \begin{equation} - \frac{\Gamma \left( \frac{s}{2} \right)}{\pi^{\frac{s}{2}} n^s} + \frac{\Gamma \left( \frac{s}{2} \right)}{\pi^{\frac{s}{2}}} + \frac{1}{n^s} = \int_0^{\infty} x^{\frac{s}{2}-1} e^{-\pi n^2 x} \,dx, \end{equation} -und finden Zeta durch die Summenbildung $\sum_{n=1}^{\infty}$ -\begin{equation} +und finden $\zeta(s)$ durch die Summenbildung über alle $n$ +\begin{align} \frac{\Gamma \left( \frac{s}{2} \right)}{\pi^{\frac{s}{2}}} \zeta(s) - = + &= \int_0^{\infty} x^{\frac{s}{2}-1} \sum_{n=1}^{\infty} e^{-\pi n^2 x} - \,dx. \label{zeta:equation:integral1} -\end{equation} -Die Summe kürzen wir ab als $\psi(x) = \sum_{n=1}^{\infty} e^{-\pi n^2 x}$. -Im Abschnitt \ref{zeta:subsec:poisson_summation} wird die poissonsche Summenformel $\sum f(n) = \sum F(n)$ bewiesen. -In unserem Problem ist $f(n) = e^{-\pi n^2 x}$ und die zugehörige Fouriertransformation $F(n)$ ist -\begin{equation} - F(n) - = - \mathcal{F} - ( - e^{-\pi n^2 x} - ) - = - \frac{1}{\sqrt{x}} - e^{\frac{-n^2 \pi}{x}}. -\end{equation} -Dadurch ergibt sich -\begin{equation}\label{zeta:equation:psi} - \sum_{n=-\infty}^{\infty} - e^{-\pi n^2 x} - = - \frac{1}{\sqrt{x}} - \sum_{n=-\infty}^{\infty} - e^{\frac{-n^2 \pi}{x}}, -\end{equation} -wobei wir die Summen so verändern müssen, dass sie bei $n=1$ beginnen und wir $\psi(x)$ erhalten als -\begin{align} - 2 - \sum_{n=1}^{\infty} - e^{-\pi n^2 x} - + - 1 - &= - \frac{1}{\sqrt{x}} - \left( - 2 - \sum_{n=1}^{\infty} - e^{\frac{-n^2 \pi}{x}} - + - 1 - \right) + \,dx\label{zeta:equation:integral1} \\ - 2 - \psi(x) - + - 1 &= - \frac{1}{\sqrt{x}} - \left( - 2 - \psi\left(\frac{1}{x}\right) - + - 1 - \right) - \\ + \int_0^{\infty} + x^{\frac{s}{2}-1} \psi(x) - &= - - \frac{1}{2} - + \frac{\psi\left(\frac{1}{x} \right)}{\sqrt{x}} - + \frac{1}{2 \sqrt{x}}.\label{zeta:equation:psi} + \,dx, \end{align} -Diese Gleichung wird später wichtig werden. - -Zunächst teilen wir nun das Integral aus \eqref{zeta:equation:integral1} auf als +wobei die Summe $\sum_{n=1}^{\infty} e^{-\pi n^2 x}$ als $\psi(x)$ abgekürzt wird. +Zunächst teilen wir nun das Integral auf in zwei Teile \begin{equation}\label{zeta:equation:integral2} \int_0^{\infty} x^{\frac{s}{2}-1} @@ -178,109 +139,20 @@ Zunächst teilen wir nun das Integral aus \eqref{zeta:equation:integral1} auf al x^{\frac{s}{2}-1} \psi(x) \,dx - }_{I_1} + }_{\displaystyle{I_1}} + \underbrace{ \int_1^{\infty} x^{\frac{s}{2}-1} \psi(x) \,dx - }_{I_2} - = - I_1 + I_2, -\end{equation} -wobei wir uns nun auf den ersten Teil $I_1$ konzentrieren werden. -Dabei setzen wir die Definition von $\psi(x)$ aus \eqref{zeta:equation:psi} ein und erhalten -\begin{align} - I_1 - = - \int_0^{1} - x^{\frac{s}{2}-1} - \psi(x) - \,dx - &= - \int_0^{1} - x^{\frac{s}{2}-1} - \left( - - \frac{1}{2} - + \frac{\psi\left(\frac{1}{x} \right)}{\sqrt{x}} - + \frac{1}{2 \sqrt{x}} - \right) - \,dx - \\ - &= - \int_0^{1} - x^{\frac{s}{2}-\frac{3}{2}} - \psi \left( \frac{1}{x} \right) - + \frac{1}{2} - \biggl( - x^{\frac{s}{2}-\frac{3}{2}} - - - x^{\frac{s}{2}-1} - \biggl) - \,dx - \\ - &= - \underbrace{ - \int_0^{1} - x^{\frac{s}{2}-\frac{3}{2}} - \psi \left( \frac{1}{x} \right) - \,dx - }_{I_3} - + - \underbrace{ - \frac{1}{2} - \int_0^1 - x^{\frac{s}{2}-\frac{3}{2}} - - - x^{\frac{s}{2}-1} - \,dx - }_{I_4}. \label{zeta:equation:integral3} -\end{align} -Dabei kann das zweite Integral $I_4$ gelöst werden als -\begin{equation} - I_4 - = - \frac{1}{2} - \int_0^1 - x^{\frac{s}{2}-\frac{3}{2}} - - - x^{\frac{s}{2}-1} - \,dx + }_{\displaystyle{I_2}} = - \frac{1}{s(s-1)}. + I_1 + I_2. \end{equation} -Das erste Integral $I_3$ aus \eqref{zeta:equation:integral3} mit $\psi \left(\frac{1}{x} \right)$ ist nicht lösbar in dieser Form. -Deshalb substituieren wir $x = \frac{1}{u}$ und $dx = -\frac{1}{u^2}du$. -Die untere Integralgrenze wechselt ebenfalls zu $x_0 = 0 \rightarrow u_0 = \infty$. -Dies ergibt -\begin{align} - I_3 - = - \int_{\infty}^{1} - \left( - \frac{1}{u} - \right)^{\frac{s}{2}-\frac{3}{2}} - \psi(u) - \frac{-du}{u^2} - &= - \int_{1}^{\infty} - \left( - \frac{1}{u} - \right)^{\frac{s}{2}-\frac{3}{2}} - \psi(u) - \frac{du}{u^2} - \\ - &= - \int_{1}^{\infty} - x^{(-1) \left(\frac{s}{2}+\frac{1}{2}\right)} - \psi(x) - \,dx, -\end{align} -wobei wir durch Multiplikation mit $(-1)$ die Integralgrenzen tauschen dürfen. -Es ist zu beachten das diese Grenzen nun identisch mit den Grenzen des zweiten Integrals von \eqref{zeta:equation:integral2} sind. -Wir setzen beide Lösungen ein in Gleichung \eqref{zeta:equation:integral3} und erhalten -\begin{equation} +Abschnitt \ref{zeta:subsubsec:intcal} beschreibt wie das Integral $I_1$ umgestellt werden kann um ebenfalls die Integrationsgrenzen $1$ und $\infty$ zu bekommen. +Die Lösung, beschrieben in Gleichung \eqref{zeta:equation:intcal_res}, lautet +\begin{equation*} I_1 = \int_0^{1} @@ -294,8 +166,8 @@ Wir setzen beide Lösungen ein in Gleichung \eqref{zeta:equation:integral3} und \,dx + \frac{1}{s(s-1)}. -\end{equation} -Dieses Resultat setzen wir wiederum ein in \eqref{zeta:equation:integral2}, um schlussendlich +\end{equation*} +Dieses Resultat setzen wir nun ein in \eqref{zeta:equation:integral2}, um schlussendlich \begin{align} \frac{\Gamma \left( \frac{s}{2} \right)}{\pi^{\frac{s}{2}}} \zeta(s) @@ -356,17 +228,21 @@ Somit haben wir die analytische Fortsetzung gefunden als \zeta(s) = \frac{\Gamma \left( \frac{1-s}{2} \right)}{\pi^{\frac{1-s}{2}}} - \zeta(1-s). + \zeta(1-s), \end{equation} -%TODO Definitionen und Gleichungen klarer unterscheiden +was einer Spiegelung an der $\Re(s) = \frac{1}{2}$ Geraden entspricht. +Eine ganz ähnliche Spiegelungseigenschaft wurde bereits in Abschnitt \ref{buch:funktionentheorie:subsection:gammareflektion} für die Gammafunktion gefunden. + +\subsection{Berechnung des Integrals $I_1 = \int_0^{1} x^{\frac{s}{2}-1} \psi(x) \,dx$} \label{zeta:subsubsec:intcal} -\subsection{Poissonsche Summenformel} \label{zeta:subsec:poisson_summation} +Ziel dieses Abschnittes ist, zu zeigen wie das Integral $I_1$ aus Gleichung \eqref{zeta:equation:integral2} durch ein neues Integral mit den Integrationsgrenzen $1$ und $\infty$ ersetzt werden kann. +Da dieser Schritt ziemlich aufwendig ist, wird er hier in einem eigenen Abschnitt behandelt. +Zunächst wird die poissonsche Summenformel hergeleitet \cite{zeta:online:poisson}, da diese verwendet werden kann um $\psi(x)$ zu berechnen. -Der Beweis für Gleichung \ref{zeta:equation:psi} folgt direkt durch die poissonsche Summenformel. -Um diese zu beweisen, berechnen wir zunächst die Fourierreihe der Dirac Delta Funktion. +Um die poissonsche Summenformel zu beweisen, berechnen wir zunächst die Fourierreihe der Dirac Delta Funktion. \begin{lemma} - Die Fourierreihe der periodischen Dirac Delta Funktion $\sum \delta(x - 2\pi k)$ ist + Die Fourierreihe der periodischen Dirac $\delta$ Funktion $\sum \delta(x - 2\pi k)$ ist \begin{equation} \label{zeta:equation:fourier_dirac} \sum_{k=-\infty}^{\infty} \delta(x - 2\pi k) @@ -437,8 +313,8 @@ Um diese zu beweisen, berechnen wir zunächst die Fourierreihe der Dirac Delta F \underbrace{ \sum_{k=-\infty}^{\infty} e^{-i 2\pi x k} - }_{\text{\eqref{zeta:equation:fourier_dirac}}} - \, dx, + }_{\displaystyle{\text{\eqref{zeta:equation:fourier_dirac}}}} + \, dx, \label{zeta:equation:1934} \end{align} und verwenden die Fouriertransformation der Dirac Funktion aus \eqref{zeta:equation:fourier_dirac} \begin{align} @@ -454,7 +330,7 @@ Um diese zu beweisen, berechnen wir zunächst die Fourierreihe der Dirac Delta F \sum_{k=-\infty}^{\infty} \delta(x + k). \end{align} - Wenn wir dies einsetzen und erhalten wir den gesuchten Beweis für die poissonsche Summenformel + Wenn wir dies einsetzen in Gleichung \eqref{zeta:equation:1934} erhalten wir \begin{equation} \sum_{k=-\infty}^{\infty} F(k) @@ -472,6 +348,190 @@ Um diese zu beweisen, berechnen wir zunächst die Fourierreihe der Dirac Delta F \, dx = \sum_{k=-\infty}^{\infty} - f(k). + f(k), \end{equation} + was der gesuchte Beweis für die poissonsche Summenformel ist. \end{proof} + +Erinnern wir uns nochmals an unser Integral aus Gleichung \eqref{zeta:equation:integral2} +\begin{align*} + I_1 + &= + \int_0^{1} + x^{\frac{s}{2}-1} + \sum_{n=1}^{\infty} + e^{-\pi n^2 x} + \,dx + \\ + &= + \int_0^{1} + x^{\frac{s}{2}-1} + \psi(x) + \,dx + . +\end{align*} + +Wir wenden nun diese poissonsche Summenformel $\sum f(n) = \sum F(n)$ an auf $\psi(x)$. +In unserem Problem ist also $f(n) = e^{-\pi n^2 x}$ und die zugehörige Fouriertransformation $F(n)$ ist +\begin{equation} + F(n) + = + \mathcal{F} + ( + e^{-\pi n^2 x} + ) + = + \frac{1}{\sqrt{x}} + e^{\frac{-n^2 \pi}{x}}. +\end{equation} +Dadurch ergibt sich +\begin{equation}\label{zeta:equation:psi} + \sum_{n=-\infty}^{\infty} + e^{-\pi n^2 x} + = + \frac{1}{\sqrt{x}} + \sum_{n=-\infty}^{\infty} + e^{\frac{-n^2 \pi}{x}}, +\end{equation} +wobei wir die Summen so verändern müssen, dass sie bei $n=1$ beginnen und wir $\psi(x)$ erhalten als +\begin{align} + 2 + \sum_{n=1}^{\infty} + e^{-\pi n^2 x} + + + 1 + &= + \frac{1}{\sqrt{x}} + \Biggl( + 2 + \sum_{n=1}^{\infty} + e^{\frac{-n^2 \pi}{x}} + + + 1 + \Biggr) + \\ + 2 + \psi(x) + + + 1 + &= + \frac{1}{\sqrt{x}} + \left( + 2 + \psi\left(\frac{1}{x}\right) + + + 1 + \right) + \\ + \psi(x) + &= + - \frac{1}{2} + + \frac{\psi\left(\frac{1}{x} \right)}{\sqrt{x}} + + \frac{1}{2 \sqrt{x}}.\label{zeta:equation:psi} +\end{align} +Diese Form von $\psi(x)$ eingesetzt in $I_1$ ergibt +\begin{align} + I_1 + = + \int_0^{1} + x^{\frac{s}{2}-1} + \psi(x) + \,dx + &= + \int_0^{1} + x^{\frac{s}{2}-1} + \Biggl( + - \frac{1}{2} + + \frac{\psi\left(\frac{1}{x} \right)}{\sqrt{x}} + + \frac{1}{2 \sqrt{x}} + \Biggr) + \,dx + \\ + &= + \int_0^{1} + x^{\frac{s}{2}-\frac{3}{2}} + \psi \left( \frac{1}{x} \right) + + \frac{1}{2} + \biggl( + x^{\frac{s}{2}-\frac{3}{2}} + - + x^{\frac{s}{2}-1} + \biggl) + \,dx + \\ + &= + \underbrace{ + \int_0^{1} + x^{\frac{s}{2}-\frac{3}{2}} + \psi \left( \frac{1}{x} \right) + \,dx + }_{\displaystyle{I_3}} + + + \underbrace{ + \frac{1}{2} + \int_0^1 + x^{\frac{s}{2}-\frac{3}{2}} + - + x^{\frac{s}{2}-1} + \,dx + }_{\displaystyle{I_4}}. \label{zeta:equation:integral3} +\end{align} +Darin kann für das zweite Integral $I_4$ eine Lösung gefunden werden als +\begin{equation} + I_4 + = + \frac{1}{2} + \int_0^1 + x^{\frac{s}{2}-\frac{3}{2}} + - + x^{\frac{s}{2}-1} + \,dx + = + \frac{1}{s(s-1)}. +\end{equation} +Das erste Integral $I_3$ aus \eqref{zeta:equation:integral3} mit $\psi \left(\frac{1}{x} \right)$ ist hingegen nicht lösbar in dieser Form. +Deshalb substituieren wir $x = \frac{1}{u}$ und $dx = -\frac{1}{u^2}du$. +Die untere Integralgrenze wechselt ebenfalls zu $x_0 = 0 \rightarrow u_0 = \infty$. +Dies ergibt +\begin{align} + I_3 + = + \int_{\infty}^{1} + \left( + \frac{1}{u} + \right)^{\frac{s}{2}-\frac{3}{2}} + \psi(u) + \frac{-du}{u^2} + &= + \int_{1}^{\infty} + \left( + \frac{1}{u} + \right)^{\frac{s}{2}-\frac{3}{2}} + \psi(u) + \frac{du}{u^2} + \\ + &= + \int_{1}^{\infty} + x^{(-1) \left(\frac{s}{2}+\frac{1}{2}\right)} + \psi(x) + \,dx, +\end{align} +wobei wir durch Multiplikation mit $(-1)$ die Integralgrenzen tauschen dürfen. +Es ist zu beachten das diese Grenzen nun identisch mit den Grenzen des zweiten Integrals $I_2$ von \eqref{zeta:equation:integral2} sind. +Wir setzen beide Lösungen in Gleichung \eqref{zeta:equation:integral3} ein und erhalten +\begin{equation} + I_1 + = + \int_0^{1} + x^{\frac{s}{2}-1} + \psi(x) + \,dx + = + \int_{1}^{\infty} + x^{(-1) \left(\frac{s}{2}+\frac{1}{2}\right)} + \psi(x) + \,dx + + + \frac{1}{s(s-1)}. \label{zeta:equation:intcal_res} +\end{equation} +Diese Form des Integrals $I_1$ hat die gewünschten Integrationsgrenzen und ein essentieller Bestandteil des Beweises der Funktionalgleichung in Abschnitt \ref{zeta:subsection:auf_ganz}. diff --git a/buch/papers/zeta/einleitung.tex b/buch/papers/zeta/einleitung.tex index 3b70531..828678d 100644 --- a/buch/papers/zeta/einleitung.tex +++ b/buch/papers/zeta/einleitung.tex @@ -1,11 +1,41 @@ \section{Einleitung} \label{zeta:section:einleitung} \rhead{Einleitung} -Die Riemannsche Zetafunktion ist für alle komplexe $s$ mit $\Re(s) > 1$ definiert als +Die Riemannsche Zetafunktion $\zeta(s)$ ist für alle komplexe $s$ mit $\Re(s) > 1$ definiert als \begin{equation}\label{zeta:equation1} \zeta(s) = \sum_{n=1}^{\infty} \frac{1}{n^s}. \end{equation} +Die Zetafunktion ist bekannt als Bestandteil der Riemannschen Vermutung, welche besagt das alle nichttrivialen Nullstellen der Zetafunktion einen Realteil von $\frac{1}{2}$ haben. +Mithilfe dieser Vermutung kann eine gute Annäherung an die Primzahlfunktion gefunden werden. +Die Primzahlfunktion steigt immer an, sobald eine Primzahl vorkommt. +Eine Darstellung davon ist in Abbildung \ref{fig:zeta:primzahlfunktion} zu finden. +Die Riemannsche Vermutung ist eines der ungelösten Millennium-Probleme der Mathematik, auf deren Lösung eine Belohnung von einer Million Dollar ausgesetzt ist \cite{zeta:online:millennium}. +Auf eine genauere Beschreibung der Riemannschen Vermutung wird im Rahmen dieses Papers nicht eingegangen. +\begin{figure} + \centering + \input{papers/zeta/images/primzahlfunktion2.tex} + \caption{Die Primzahlfunktion von $0$ bis $30$.} + \label{fig:zeta:primzahlfunktion} +\end{figure} +Der grundlegende Zusammenhang der Primzahlen und der Zetafunktion wird im ersten Abschnitt \ref{zeta:section:eulerprodukt} über das Eulerprodukt gezeigt. +Danach folgt die Verbindung zur bereits bekannten Gammafunktion in Abschnitt \ref{zeta:section:zusammenhang_mit_gammafunktion}. +Schlussendlich folgt die Beschreibung der analytischen Fortsetzung die gesamte komplexe Ebene in Abschnitt \ref{zeta:section:analytische_fortsetzung}. + +Diese analytische Fortsetzung wird für die Riemannsche Vermutung benötigt, ermöglicht aber auch andere interessante Aussagen. +So findet sich zum Beispiel immer wieder die aberwitzige Behauptung, das die Summe aller natürlichen Zahlen +\begin{equation*} + \sum_{n=1}^{\infty} n + = + \sum_{n=1}^{\infty} + \frac{1}{n^{-1}} + = + -\frac{1}{12} +\end{equation*} +sei. +Obwohl diese Behauptung offensichtlich falsch ist, hat sie doch ihre Berechtigung, wie durch die analytische Fortsetzung gezeigt werden wird. + +Die folgenden mathematischen Herleitungen sind, sofern nicht anders gekennzeichnet, eigene Darstellungen basierend auf den überaus umfangreichen Wikipedia-Artikeln auf Deutsch \cite{zeta:online:wiki_de} und Englisch \cite{zeta:online:wiki_en} sowie einer Video-Playlist \cite{zeta:online:mryoumath}. diff --git a/buch/papers/zeta/euler_product.tex b/buch/papers/zeta/euler_product.tex index a6ed512..9c08dd2 100644 --- a/buch/papers/zeta/euler_product.tex +++ b/buch/papers/zeta/euler_product.tex @@ -1,9 +1,9 @@ \section{Eulerprodukt} \label{zeta:section:eulerprodukt} \rhead{Eulerprodukt} -Das Eulerprodukt stellt die Verbindung der Zetafunktion und der Primzahlen her. -Diese Verbindung ist sehr wichtig, da durch sie eine Aussage zur Primzahlverteilung gemacht werden kann. -Die Verteilung der Primzahlen ist Gegenstand der Riemannschen Vermutung, welche eines der grössten ungelösten Probleme der Mathematik ist. +Das Eulerprodukt stellt die gesuchte Verbindung der Zetafunktion und der Primzahlen her. +Wie der Name bereits sagt, wurde das Eulerprodukt bereits 1727 von Euler entdeckt. +Um daraus die Riemannsche Vermutung herzuleiten, wäre aber noch einiges mehr nötig. \begin{satz} Für alle Zahlen $s$ mit $\Re(s) > 1$ ist die Zetafunktion identisch mit dem unendlichen Eulerprodukt @@ -28,9 +28,9 @@ Die Verteilung der Primzahlen ist Gegenstand der Riemannschen Vermutung, welche = \prod_{p \in P} \sum_{k_i=0}^{\infty} - \left( + \biggl( \frac{1}{p_i^s} - \right)^{k_i} + \biggr)^{k_i} = \prod_{p \in P} \sum_{k_i=0}^{\infty} @@ -53,33 +53,34 @@ Die Verteilung der Primzahlen ist Gegenstand der Riemannschen Vermutung, welche \sum_{k_1=0}^{\infty} \sum_{k_2=0}^{\infty} \ldots - \left( + \biggl( \frac{1}{p_1^{k_1}} \frac{1}{p_2^{k_2}} \ldots - \right)^s. + \biggr)^s. \label{zeta:equation:eulerprodukt2} \end{align} Der Fundamentalsatz der Arithmetik (Primfaktorzerlegung) besagt, dass jede beliebige Zahl $n \in \mathbb{N}$ durch eine eindeutige Primfaktorzerlegung beschrieben werden kann \begin{equation} n = \prod_i p_i^{k_i} \quad \forall \quad n \in \mathbb{N}. \end{equation} - Jeder Summand der Summen in \eqref{zeta:equation:eulerprodukt2} ist somit eine Zahl $n$. - Da die Summen alle möglichen Kombinationen von Exponenten und Primzahlen in \eqref{zeta:equation:eulerprodukt2} enthält haben wir + Jeder Summand der Summen in \eqref{zeta:equation:eulerprodukt2} ist somit der Kehrwert genau einer natürlichen Zahl $n \in \mathbb{N}$. + Da die Summen alle möglichen Kombinationen von Exponenten und Primzahlen in \eqref{zeta:equation:eulerprodukt2} enthält, haben wir \begin{equation} \sum_{k_1=0}^{\infty} \sum_{k_2=0}^{\infty} \ldots - \left( + \biggl( \frac{1}{p_1^{k_1}} \frac{1}{p_2^{k_2}} \ldots - \right)^s + \biggr)^s = \sum_{n=1}^\infty \frac{1}{n^s} = - \zeta(s) + \zeta(s), \end{equation} + wodurch das Eulerprodukt bewiesen ist. \end{proof} diff --git a/buch/papers/zeta/fazit.tex b/buch/papers/zeta/fazit.tex new file mode 100644 index 0000000..027f324 --- /dev/null +++ b/buch/papers/zeta/fazit.tex @@ -0,0 +1,94 @@ +\section{Der Wert $\zeta(-1)$} \label{zeta:section:fazit} +\rhead{Der Wert $\zeta(-1)$} + +Ganz zu Beginn dieses Papers wurde die Behauptung erwähnt, dass die Summe aller natürlichen Zahlen $-\frac{1}{12}$ sei. +Diese Summe ist nichts anderes als die Zetafunktion am Wert $s=-1$. +Da wir die analytische Fortsetzung mit der Funktionalgleichung \eqref{zeta:equation:functional} gefunden haben, können wir den Wert $s=-1$ einsetzen und erhalten +\begin{align*} + \zeta(s) + &= + \frac{\Gamma \left( \frac{1-s}{2} \right)}{\pi^{\frac{1-s}{2}}} + \zeta(1-s) + \frac{\pi^{\frac{s}{2}}}{\Gamma \left( \frac{s}{2} \right)} + \\ + \zeta(-1) + &= + \frac{\Gamma(1)}{\pi} + \zeta(2) + \frac{\pi^{-\frac{1}{2}}}{\Gamma \left( -\frac{1}{2} \right)}. +\end{align*} +Also fehlen uns drei Werte, $\zeta(2)$, $\Gamma(1)$ und $\Gamma(-\frac{1}{2})$. + +Zunächst konzentrieren wir uns auf $\zeta(2)$, welches im konvergenten Bereich der Reihe liegt und auch bekannt ist als das Basler Problem. +Wir lösen das Basler Problem \cite{zeta:online:basel} mithilfe der parsevalschen Gleichung \cite{zeta:online:pars} +\begin{align} + \int_{-\pi}^{\pi} |f(x)|^2 dx + &= + 2\pi \sum_{n=-\infty}^{\infty} |c_n|^2 \\ + c_n + &= + \frac{1}{2\pi} + \int_{-\pi}^{\pi}f(x)e^{-inx} dx, +\end{align} +welche besagt dass die Summe der quadrierten Fourierkoeffizienten einer Funktion identisch ist mit dem Integral der quadrierten Funktion. +Wenn wir dies für $f(x) = x$ auswerten erhalten wir +\begin{align} + c_n + &= + \begin{cases} + \frac{(-1)^n}{n} i, & \text{for } n\neq0, \\ + 0, & \text{for } n=0 + \end{cases} + \\ + \int_{-\pi}^{\pi} x^2 dx + &= + 2\pi \sum_{n=-\infty}^{\infty} |c_n|^2 + = + 4\pi \underbrace{\sum_{n=1}^{\infty} \frac{1}{n^2}}_{\displaystyle{\zeta(2)}}. +\end{align} +Durch einfaches Umstellen erhalten wir somit die Lösung des Basler Problems als +\begin{equation} + \zeta(2) = \sum_{n=1}^{\infty} \frac{1}{n^2} = \frac{1}{4\pi} + \int_{-\pi}^{\pi} x^2 dx + = \frac{\pi^2}{6}. +\end{equation} + +Als nächstes berechnen wir $\Gamma(1)$ und $\Gamma(-\frac{1}{2})$ mithilfe der Integraldefinition der Gammafunktion (Definition \ref{buch:rekursion:def:gamma}). +Da das Integral für $\Gamma(-\frac{1}{2})$ nicht konvergiert, wird die Reflektionsformel aus \ref{buch:funktionentheorie:subsection:gammareflektion} verwendet, welche das konvergierende Integral von $\Gamma(\frac{3}{2})$ verwendet. +Es ergeben sich die Werte +\begin{align*} + \Gamma(1) + &= 1\\ + \Gamma\biggl(-\frac{1}{2}\biggr) + &= \frac{\pi}{\sin\left(-\frac{\pi}{2}\right) + \Gamma\left(\frac{3}{2}\right)} + = -\frac{\sqrt{\pi}}{2}. +\end{align*} + +Wenn wir diese Werte in die Funktionalgleichung einsetzen, erhalten wir das gewünschte Ergebnis +\begin{align*} + \zeta(-1) + &= + \frac{\Gamma(1)}{\pi} + \zeta(2) + \frac{\pi^{-\frac{1}{2}}}{\Gamma \left( -\frac{1}{2} \right)} + \\ + &= + \frac{1}{\pi} + \frac{\pi^2}{6} + \frac{\pi^{-\frac{1}{2}}}{ + -\frac{\sqrt{\pi}}{2}} + \\ + &= + -\frac{1}{12}. +\end{align*} + +Weiter wurde zu Beginn dieses Papers auf die Riemannsche Vermutung hingewiesen, wonach alle nichttrivialen Nullstellen der Zetafunktion auf der $\Re(s)=\frac{1}{2}$ Geraden liegen. +Abbildung \ref{zeta:fig:einzweitel} zeigt die Funktionswerte dieser Geraden. +\begin{figure} + \centering + \input{papers/zeta/images/zetaplot.tex} + \caption{Die komplexen Werte der Zetafunktion für die kritische Gerade $\Re(s)=\frac{1}{2}$ im Bereich $\Im(s) = 0\dots40$. + Klar sichtbar sind die immer wiederkehrenden Nullstellen, wie sie Gegenstand der Riemannschen Vermutung sind.} + \label{zeta:fig:einzweitel} +\end{figure} diff --git a/buch/papers/zeta/images/Makefile b/buch/papers/zeta/images/Makefile new file mode 100644 index 0000000..611662d --- /dev/null +++ b/buch/papers/zeta/images/Makefile @@ -0,0 +1,10 @@ +# +# Makefile to build images +# +all: primzahlfunktion2.pdf zetaplot.pdf + +primzahlfunktion2.pdf: primzahlfunktion2.tex + pdflatex primzahlfunktion2.tex + +zetaplot.pdf: zetaplot.tex zetapath.tex + pdflatex zetaplot.tex diff --git a/buch/papers/zeta/continuation_overview.tikz.tex b/buch/papers/zeta/images/continuation_overview.tikz.tex index 836ab1d..836ab1d 100644 --- a/buch/papers/zeta/continuation_overview.tikz.tex +++ b/buch/papers/zeta/images/continuation_overview.tikz.tex diff --git a/buch/papers/zeta/images/primzahlfunktion.pgf b/buch/papers/zeta/images/primzahlfunktion.pgf new file mode 100644 index 0000000..7d4f4fc --- /dev/null +++ b/buch/papers/zeta/images/primzahlfunktion.pgf @@ -0,0 +1,505 @@ +%% Creator: Matplotlib, PGF backend +%% +%% To include the figure in your LaTeX document, write +%% \input{<filename>.pgf} +%% +%% Make sure the required packages are loaded in your preamble +%% \usepackage{pgf} +%% +%% and, on pdftex +%% \usepackage[utf8]{inputenc}\DeclareUnicodeCharacter{2212}{-} +%% +%% or, on luatex 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a/buch/papers/zeta/images/primzahlfunktion2.tex b/buch/papers/zeta/images/primzahlfunktion2.tex new file mode 100644 index 0000000..7425ce5 --- /dev/null +++ b/buch/papers/zeta/images/primzahlfunktion2.tex @@ -0,0 +1,63 @@ +% +% primzahlfunktion2.tex -- Primzahlfunktion, alternativer Vorschlag +% +% (c) 2021 Prof Dr Andreas Müller, OST Ostschweizer Fachhochschule +% +\documentclass[tikz]{standalone} +\usepackage{amsmath} +\usepackage{times} +\usepackage{txfonts} +\usepackage{pgfplots} +\usepackage{csvsimple} +\usetikzlibrary{arrows,intersections,math} +\begin{document} +\def\skala{1} +\begin{tikzpicture}[>=latex,thick,scale=\skala] + +\def\dx{0.38} +\def\dy{0.5} + +\foreach \x in {1,...,30}{ + \draw[color=gray!20] ({\x*\dx},0) -- ({\x*\dx},{10.5*\dy}); +} +\foreach \y in {1,...,10}{ + \draw[color=gray!20] (0,{\y*\dy}) -- ({30.5*\dx},{\y*\dy}); +} + +\draw[->] (-0.1,0) -- ({30.8*\dx},0) coordinate[label={$x$}]; +\draw[->] (0,-0.1) -- (0,{10.9*\dy}) coordinate[label={right:$\pi(x)$}]; + +\def\segment#1#2#3{ + %\draw[line width=0.1pt] ({#3*\dx},0) -- ({#3*\dx},{#2*\dy}); + \draw[color=blue,line width=1.4pt] + ({#1*\dx},{#2*\dy}) -- ({#3*\dx},{#2*\dy}); + \draw[color=blue,line width=0.3pt] + ({#3*\dx},{#2*\dy}) -- ({#3*\dx},{(#2+1)*\dy}); + \draw ({#3*\dx},-0.1) -- ({#3*\dx},0.1); + \node at ({(#3)*\dx},-0.1) [below] {$#3\mathstrut$}; +} + +\foreach \y in {2,4,...,10}{ + \draw (-0.1,{\y*\dy}) -- (0.1,{\y*\dy}); + \node at (-0.1,{\y*\dy}) [left] {$\y\mathstrut$}; +} + +\begin{scope} +\clip (0,-0.5) rectangle ({30*\dx},{10.1*\dy}); + +\segment{0}{0}{2} +\segment{2}{1}{3} +\segment{3}{2}{5} +\segment{5}{3}{7} +\segment{7}{4}{11} +\segment{11}{5}{13} +\segment{13}{6}{17} +\segment{17}{7}{19} +\segment{19}{8}{23} +\segment{23}{9}{29} +\segment{29}{10}{31} +\end{scope} + +\end{tikzpicture} +\end{document} + diff --git a/buch/papers/zeta/images/primzahlfunktion_paper.pgf b/buch/papers/zeta/images/primzahlfunktion_paper.pgf new file mode 100644 index 0000000..b9d67d3 --- /dev/null +++ b/buch/papers/zeta/images/primzahlfunktion_paper.pgf @@ -0,0 +1,505 @@ +%% Creator: Matplotlib, PGF backend +%% +%% To include the figure in your LaTeX document, write +%% \input{<filename>.pgf} +%% +%% Make sure the required packages are loaded in your preamble +%% \usepackage{pgf} +%% +%% and, on pdftex +%% \usepackage[utf8]{inputenc}\DeclareUnicodeCharacter{2212}{-} +%% +%% or, on luatex and xetex +%% \usepackage{unicode-math} +%% +%% Figures using additional raster images can only be included by \input if +%% they are in the same directory as the main LaTeX file. For loading figures +%% from other directories you can use the `import` package +%% \usepackage{import} +%% +%% and then include the figures with +%% \import{<path to file>}{<filename>.pgf} +%% +%% Matplotlib used the following preamble +%% +\begingroup% +\makeatletter% +\begin{pgfpicture}% +\pgfpathrectangle{\pgfpointorigin}{\pgfqpoint{5.440000in}{3.480000in}}% +\pgfusepath{use as bounding box, clip}% +\begin{pgfscope}% +\pgfsetbuttcap% +\pgfsetmiterjoin% +\definecolor{currentfill}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetfillcolor{currentfill}% +\pgfsetlinewidth{0.000000pt}% +\definecolor{currentstroke}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetstrokecolor{currentstroke}% +\pgfsetdash{}{0pt}% +\pgfpathmoveto{\pgfqpoint{0.000000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{5.440000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{5.440000in}{3.480000in}}% +\pgfpathlineto{\pgfqpoint{0.000000in}{3.480000in}}% +\pgfpathclose% +\pgfusepath{fill}% +\end{pgfscope}% +\begin{pgfscope}% 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a/buch/papers/zeta/images/zeta_re_-1_plot.pgf b/buch/papers/zeta/images/zeta_re_-1_plot.pgf new file mode 100644 index 0000000..dd15ba1 --- /dev/null +++ b/buch/papers/zeta/images/zeta_re_-1_plot.pgf @@ -0,0 +1,1147 @@ +%% Creator: Matplotlib, PGF backend +%% +%% To include the figure in your LaTeX document, write +%% \input{<filename>.pgf} +%% +%% Make sure the required packages are loaded in your preamble +%% \usepackage{pgf} +%% +%% and, on pdftex +%% \usepackage[utf8]{inputenc}\DeclareUnicodeCharacter{2212}{-} +%% +%% or, on luatex and xetex +%% \usepackage{unicode-math} +%% +%% Figures using additional raster images can only be included by \input if +%% they are in the same directory as the main LaTeX file. For loading figures +%% from other directories you can use the `import` package +%% \usepackage{import} +%% +%% and then include the figures with +%% \import{<path to file>}{<filename>.pgf} +%% +%% Matplotlib used the following preamble +%% +\begingroup% +\makeatletter% +\begin{pgfpicture}% +\pgfpathrectangle{\pgfpointorigin}{\pgfqpoint{6.400000in}{4.800000in}}% +\pgfusepath{use as bounding box, clip}% +\begin{pgfscope}% +\pgfsetbuttcap% +\pgfsetmiterjoin% +\definecolor{currentfill}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetfillcolor{currentfill}% +\pgfsetlinewidth{0.000000pt}% +\definecolor{currentstroke}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetstrokecolor{currentstroke}% +\pgfsetdash{}{0pt}% +\pgfpathmoveto{\pgfqpoint{0.000000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{6.400000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{6.400000in}{4.800000in}}% +\pgfpathlineto{\pgfqpoint{0.000000in}{4.800000in}}% +\pgfpathclose% +\pgfusepath{fill}% +\end{pgfscope}% +\begin{pgfscope}% 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b/buch/papers/zeta/images/zeta_re_0.5_paper.pgf new file mode 100644 index 0000000..44fffce --- /dev/null +++ b/buch/papers/zeta/images/zeta_re_0.5_paper.pgf @@ -0,0 +1,1137 @@ +%% Creator: Matplotlib, PGF backend +%% +%% To include the figure in your LaTeX document, write +%% \input{<filename>.pgf} +%% +%% Make sure the required packages are loaded in your preamble +%% \usepackage{pgf} +%% +%% and, on pdftex +%% \usepackage[utf8]{inputenc}\DeclareUnicodeCharacter{2212}{-} +%% +%% or, on luatex and xetex +%% \usepackage{unicode-math} +%% +%% Figures using additional raster images can only be included by \input if +%% they are in the same directory as the main LaTeX file. For loading figures +%% from other directories you can use the `import` package +%% \usepackage{import} +%% +%% and then include the figures with +%% \import{<path to file>}{<filename>.pgf} +%% +%% Matplotlib used the following preamble +%% +\begingroup% +\makeatletter% +\begin{pgfpicture}% +\pgfpathrectangle{\pgfpointorigin}{\pgfqpoint{3.700000in}{3.100000in}}% +\pgfusepath{use as bounding box, clip}% +\begin{pgfscope}% +\pgfsetbuttcap% +\pgfsetmiterjoin% +\definecolor{currentfill}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetfillcolor{currentfill}% +\pgfsetlinewidth{0.000000pt}% +\definecolor{currentstroke}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetstrokecolor{currentstroke}% +\pgfsetdash{}{0pt}% +\pgfpathmoveto{\pgfqpoint{0.000000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{3.700000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{3.700000in}{3.100000in}}% +\pgfpathlineto{\pgfqpoint{0.000000in}{3.100000in}}% +\pgfpathclose% +\pgfusepath{fill}% +\end{pgfscope}% +\begin{pgfscope}% 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For loading figures +%% from other directories you can use the `import` package +%% \usepackage{import} +%% +%% and then include the figures with +%% \import{<path to file>}{<filename>.pgf} +%% +%% Matplotlib used the following preamble +%% +\begingroup% +\makeatletter% +\begin{pgfpicture}% +\pgfpathrectangle{\pgfpointorigin}{\pgfqpoint{6.400000in}{4.800000in}}% +\pgfusepath{use as bounding box, clip}% +\begin{pgfscope}% +\pgfsetbuttcap% +\pgfsetmiterjoin% +\definecolor{currentfill}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetfillcolor{currentfill}% +\pgfsetlinewidth{0.000000pt}% +\definecolor{currentstroke}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetstrokecolor{currentstroke}% +\pgfsetdash{}{0pt}% +\pgfpathmoveto{\pgfqpoint{0.000000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{6.400000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{6.400000in}{4.800000in}}% +\pgfpathlineto{\pgfqpoint{0.000000in}{4.800000in}}% +\pgfpathclose% +\pgfusepath{fill}% +\end{pgfscope}% +\begin{pgfscope}% 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+\endgroup% diff --git a/buch/papers/zeta/images/zeta_re_0_plot.pgf b/buch/papers/zeta/images/zeta_re_0_plot.pgf new file mode 100644 index 0000000..29a844e --- /dev/null +++ b/buch/papers/zeta/images/zeta_re_0_plot.pgf @@ -0,0 +1,1242 @@ +%% Creator: Matplotlib, PGF backend +%% +%% To include the figure in your LaTeX document, write +%% \input{<filename>.pgf} +%% +%% Make sure the required packages are loaded in your preamble +%% \usepackage{pgf} +%% +%% and, on pdftex +%% \usepackage[utf8]{inputenc}\DeclareUnicodeCharacter{2212}{-} +%% +%% or, on luatex and xetex +%% \usepackage{unicode-math} +%% +%% Figures using additional raster images can only be included by \input if +%% they are in the same directory as the main LaTeX file. For loading figures +%% from other directories you can use the `import` package +%% \usepackage{import} +%% +%% and then include the figures with +%% \import{<path to file>}{<filename>.pgf} +%% +%% Matplotlib used the following preamble +%% +\begingroup% +\makeatletter% +\begin{pgfpicture}% +\pgfpathrectangle{\pgfpointorigin}{\pgfqpoint{6.400000in}{4.800000in}}% +\pgfusepath{use as bounding box, clip}% +\begin{pgfscope}% +\pgfsetbuttcap% +\pgfsetmiterjoin% +\definecolor{currentfill}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetfillcolor{currentfill}% +\pgfsetlinewidth{0.000000pt}% +\definecolor{currentstroke}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetstrokecolor{currentstroke}% +\pgfsetdash{}{0pt}% +\pgfpathmoveto{\pgfqpoint{0.000000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{6.400000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{6.400000in}{4.800000in}}% +\pgfpathlineto{\pgfqpoint{0.000000in}{4.800000in}}% +\pgfpathclose% +\pgfusepath{fill}% +\end{pgfscope}% +\begin{pgfscope}% 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+\pgfpathlineto{\pgfqpoint{0.800000in}{4.224000in}}% +\pgfusepath{stroke}% +\end{pgfscope}% +\begin{pgfscope}% +\pgfsetrectcap% +\pgfsetmiterjoin% +\pgfsetlinewidth{0.803000pt}% +\definecolor{currentstroke}{rgb}{0.000000,0.000000,0.000000}% +\pgfsetstrokecolor{currentstroke}% +\pgfsetdash{}{0pt}% +\pgfpathmoveto{\pgfqpoint{5.760000in}{0.528000in}}% +\pgfpathlineto{\pgfqpoint{5.760000in}{4.224000in}}% +\pgfusepath{stroke}% +\end{pgfscope}% +\begin{pgfscope}% +\pgfsetrectcap% +\pgfsetmiterjoin% +\pgfsetlinewidth{0.803000pt}% +\definecolor{currentstroke}{rgb}{0.000000,0.000000,0.000000}% +\pgfsetstrokecolor{currentstroke}% +\pgfsetdash{}{0pt}% +\pgfpathmoveto{\pgfqpoint{0.800000in}{0.528000in}}% +\pgfpathlineto{\pgfqpoint{5.760000in}{0.528000in}}% +\pgfusepath{stroke}% +\end{pgfscope}% +\begin{pgfscope}% +\pgfsetrectcap% +\pgfsetmiterjoin% +\pgfsetlinewidth{0.803000pt}% +\definecolor{currentstroke}{rgb}{0.000000,0.000000,0.000000}% +\pgfsetstrokecolor{currentstroke}% +\pgfsetdash{}{0pt}% +\pgfpathmoveto{\pgfqpoint{0.800000in}{4.224000in}}% +\pgfpathlineto{\pgfqpoint{5.760000in}{4.224000in}}% +\pgfusepath{stroke}% +\end{pgfscope}% +\end{pgfpicture}% +\makeatother% +\endgroup% diff --git a/buch/papers/zeta/images/zetapath.tex b/buch/papers/zeta/images/zetapath.tex new file mode 100644 index 0000000..75e1522 --- /dev/null +++ b/buch/papers/zeta/images/zetapath.tex @@ -0,0 +1,2003 @@ +\def\zetapath{ + ({-1.4604*\dx},{0.0000*\dy}) + -- ({-1.4572*\dx},{-0.0783*\dy}) + -- ({-1.4476*\dx},{-0.1559*\dy}) + -- ({-1.4319*\dx},{-0.2320*\dy}) + -- ({-1.4104*\dx},{-0.3058*\dy}) + -- ({-1.3834*\dx},{-0.3769*\dy}) + -- ({-1.3514*\dx},{-0.4446*\dy}) + -- ({-1.3149*\dx},{-0.5085*\dy}) + -- ({-1.2745*\dx},{-0.5682*\dy}) + -- ({-1.2308*\dx},{-0.6235*\dy}) + -- ({-1.1843*\dx},{-0.6742*\dy}) + -- ({-1.1358*\dx},{-0.7202*\dy}) + -- ({-1.0856*\dx},{-0.7617*\dy}) + -- ({-1.0344*\dx},{-0.7985*\dy}) + -- ({-0.9826*\dx},{-0.8309*\dy}) + -- ({-0.9306*\dx},{-0.8591*\dy}) + -- ({-0.8788*\dx},{-0.8833*\dy}) + -- ({-0.8275*\dx},{-0.9037*\dy}) + -- ({-0.7770*\dx},{-0.9205*\dy}) + -- ({-0.7275*\dx},{-0.9341*\dy}) + -- ({-0.6792*\dx},{-0.9446*\dy}) + -- ({-0.6322*\dx},{-0.9525*\dy}) + -- ({-0.5867*\dx},{-0.9578*\dy}) + -- ({-0.5427*\dx},{-0.9609*\dy}) + -- ({-0.5002*\dx},{-0.9620*\dy}) + -- ({-0.4593*\dx},{-0.9613*\dy}) + -- ({-0.4200*\dx},{-0.9589*\dy}) + -- ({-0.3823*\dx},{-0.9552*\dy}) + -- ({-0.3462*\dx},{-0.9502*\dy}) + -- ({-0.3116*\dx},{-0.9441*\dy}) + -- ({-0.2785*\dx},{-0.9371*\dy}) + -- ({-0.2469*\dx},{-0.9292*\dy}) + -- ({-0.2167*\dx},{-0.9206*\dy}) + -- ({-0.1878*\dx},{-0.9114*\dy}) + -- ({-0.1603*\dx},{-0.9017*\dy}) + -- ({-0.1340*\dx},{-0.8916*\dy}) + -- ({-0.1089*\dx},{-0.8811*\dy}) + -- ({-0.0849*\dx},{-0.8703*\dy}) + -- ({-0.0621*\dx},{-0.8593*\dy}) + -- ({-0.0402*\dx},{-0.8481*\dy}) + -- ({-0.0194*\dx},{-0.8367*\dy}) + -- ({0.0004*\dx},{-0.8253*\dy}) + -- ({0.0194*\dx},{-0.8137*\dy}) + -- ({0.0375*\dx},{-0.8022*\dy}) + -- ({0.0549*\dx},{-0.7906*\dy}) + -- ({0.0714*\dx},{-0.7790*\dy}) + -- ({0.0872*\dx},{-0.7675*\dy}) + -- ({0.1024*\dx},{-0.7560*\dy}) + -- ({0.1168*\dx},{-0.7446*\dy}) + -- ({0.1307*\dx},{-0.7333*\dy}) + -- ({0.1439*\dx},{-0.7221*\dy}) + -- ({0.1566*\dx},{-0.7110*\dy}) + -- ({0.1688*\dx},{-0.7000*\dy}) + -- ({0.1805*\dx},{-0.6890*\dy}) + -- ({0.1917*\dx},{-0.6783*\dy}) + -- ({0.2024*\dx},{-0.6676*\dy}) + -- ({0.2127*\dx},{-0.6571*\dy}) + -- ({0.2226*\dx},{-0.6467*\dy}) + -- ({0.2321*\dx},{-0.6364*\dy}) + -- ({0.2412*\dx},{-0.6263*\dy}) + -- ({0.2500*\dx},{-0.6163*\dy}) + -- ({0.2585*\dx},{-0.6064*\dy}) + -- ({0.2666*\dx},{-0.5967*\dy}) + -- ({0.2745*\dx},{-0.5871*\dy}) + -- ({0.2820*\dx},{-0.5777*\dy}) + -- ({0.2893*\dx},{-0.5684*\dy}) + -- ({0.2963*\dx},{-0.5592*\dy}) + -- ({0.3031*\dx},{-0.5501*\dy}) + -- ({0.3096*\dx},{-0.5412*\dy}) + -- ({0.3159*\dx},{-0.5324*\dy}) + -- ({0.3220*\dx},{-0.5237*\dy}) + -- ({0.3279*\dx},{-0.5152*\dy}) + -- ({0.3336*\dx},{-0.5067*\dy}) + -- ({0.3391*\dx},{-0.4984*\dy}) + -- ({0.3445*\dx},{-0.4902*\dy}) + -- ({0.3496*\dx},{-0.4821*\dy}) + -- ({0.3546*\dx},{-0.4742*\dy}) + -- ({0.3595*\dx},{-0.4663*\dy}) + -- ({0.3642*\dx},{-0.4586*\dy}) + -- ({0.3687*\dx},{-0.4510*\dy}) + -- ({0.3732*\dx},{-0.4434*\dy}) + -- ({0.3774*\dx},{-0.4360*\dy}) + -- ({0.3816*\dx},{-0.4287*\dy}) + -- ({0.3857*\dx},{-0.4214*\dy}) + -- ({0.3896*\dx},{-0.4143*\dy}) + -- ({0.3934*\dx},{-0.4073*\dy}) + -- ({0.3972*\dx},{-0.4003*\dy}) + -- ({0.4008*\dx},{-0.3935*\dy}) + -- ({0.4043*\dx},{-0.3867*\dy}) + -- ({0.4078*\dx},{-0.3800*\dy}) + -- ({0.4111*\dx},{-0.3734*\dy}) + -- ({0.4144*\dx},{-0.3669*\dy}) + -- ({0.4176*\dx},{-0.3605*\dy}) + -- ({0.4207*\dx},{-0.3541*\dy}) + -- ({0.4237*\dx},{-0.3478*\dy}) + -- ({0.4267*\dx},{-0.3416*\dy}) + -- ({0.4296*\dx},{-0.3355*\dy}) + -- ({0.4324*\dx},{-0.3294*\dy}) + -- ({0.4352*\dx},{-0.3234*\dy}) + -- ({0.4379*\dx},{-0.3175*\dy}) + -- ({0.4405*\dx},{-0.3116*\dy}) + -- ({0.4431*\dx},{-0.3059*\dy}) + -- ({0.4457*\dx},{-0.3001*\dy}) + -- ({0.4482*\dx},{-0.2945*\dy}) + -- ({0.4506*\dx},{-0.2889*\dy}) + -- ({0.4530*\dx},{-0.2833*\dy}) + -- ({0.4554*\dx},{-0.2778*\dy}) + -- ({0.4577*\dx},{-0.2724*\dy}) + -- ({0.4599*\dx},{-0.2670*\dy}) + -- ({0.4622*\dx},{-0.2617*\dy}) + -- ({0.4643*\dx},{-0.2565*\dy}) + -- ({0.4665*\dx},{-0.2513*\dy}) + -- ({0.4686*\dx},{-0.2461*\dy}) + -- ({0.4707*\dx},{-0.2410*\dy}) + -- ({0.4727*\dx},{-0.2359*\dy}) + -- ({0.4747*\dx},{-0.2309*\dy}) + -- ({0.4767*\dx},{-0.2259*\dy}) + -- ({0.4787*\dx},{-0.2210*\dy}) + -- ({0.4806*\dx},{-0.2161*\dy}) + -- ({0.4825*\dx},{-0.2113*\dy}) + -- ({0.4844*\dx},{-0.2065*\dy}) + -- ({0.4862*\dx},{-0.2018*\dy}) + -- ({0.4880*\dx},{-0.1971*\dy}) + -- ({0.4898*\dx},{-0.1924*\dy}) + -- ({0.4916*\dx},{-0.1878*\dy}) + -- ({0.4934*\dx},{-0.1832*\dy}) + -- ({0.4951*\dx},{-0.1786*\dy}) + -- ({0.4968*\dx},{-0.1741*\dy}) + -- ({0.4985*\dx},{-0.1696*\dy}) + -- ({0.5002*\dx},{-0.1652*\dy}) + -- ({0.5019*\dx},{-0.1608*\dy}) + -- ({0.5035*\dx},{-0.1564*\dy}) + -- ({0.5052*\dx},{-0.1521*\dy}) + -- ({0.5068*\dx},{-0.1478*\dy}) + -- ({0.5084*\dx},{-0.1435*\dy}) + -- ({0.5100*\dx},{-0.1392*\dy}) + -- ({0.5116*\dx},{-0.1350*\dy}) + -- ({0.5132*\dx},{-0.1308*\dy}) + -- ({0.5147*\dx},{-0.1267*\dy}) + -- ({0.5163*\dx},{-0.1226*\dy}) + -- ({0.5178*\dx},{-0.1185*\dy}) + -- ({0.5193*\dx},{-0.1144*\dy}) + -- ({0.5208*\dx},{-0.1103*\dy}) + -- ({0.5224*\dx},{-0.1063*\dy}) + -- ({0.5239*\dx},{-0.1023*\dy}) + -- ({0.5254*\dx},{-0.0984*\dy}) + -- ({0.5268*\dx},{-0.0944*\dy}) + -- ({0.5283*\dx},{-0.0905*\dy}) + -- ({0.5298*\dx},{-0.0866*\dy}) + -- ({0.5313*\dx},{-0.0827*\dy}) + -- ({0.5327*\dx},{-0.0789*\dy}) + -- ({0.5342*\dx},{-0.0751*\dy}) + -- ({0.5357*\dx},{-0.0713*\dy}) + -- ({0.5371*\dx},{-0.0675*\dy}) + -- ({0.5386*\dx},{-0.0637*\dy}) + -- ({0.5400*\dx},{-0.0600*\dy}) + -- ({0.5414*\dx},{-0.0563*\dy}) + -- ({0.5429*\dx},{-0.0526*\dy}) + -- ({0.5443*\dx},{-0.0489*\dy}) + -- ({0.5458*\dx},{-0.0453*\dy}) + -- ({0.5472*\dx},{-0.0416*\dy}) + -- ({0.5486*\dx},{-0.0380*\dy}) + -- ({0.5501*\dx},{-0.0344*\dy}) + -- ({0.5515*\dx},{-0.0308*\dy}) + -- ({0.5529*\dx},{-0.0272*\dy}) + -- ({0.5544*\dx},{-0.0237*\dy}) + -- ({0.5558*\dx},{-0.0202*\dy}) + -- ({0.5572*\dx},{-0.0167*\dy}) + -- ({0.5587*\dx},{-0.0132*\dy}) + -- ({0.5601*\dx},{-0.0097*\dy}) + -- ({0.5615*\dx},{-0.0062*\dy}) + -- ({0.5630*\dx},{-0.0028*\dy}) + -- ({0.5644*\dx},{0.0006*\dy}) + -- ({0.5659*\dx},{0.0041*\dy}) + -- ({0.5673*\dx},{0.0075*\dy}) + -- ({0.5688*\dx},{0.0108*\dy}) + -- ({0.5702*\dx},{0.0142*\dy}) + -- ({0.5717*\dx},{0.0176*\dy}) + -- ({0.5731*\dx},{0.0209*\dy}) + -- ({0.5746*\dx},{0.0242*\dy}) + -- ({0.5761*\dx},{0.0275*\dy}) + -- ({0.5776*\dx},{0.0308*\dy}) + -- ({0.5790*\dx},{0.0341*\dy}) + -- ({0.5805*\dx},{0.0374*\dy}) + -- ({0.5820*\dx},{0.0407*\dy}) + -- ({0.5835*\dx},{0.0439*\dy}) + -- ({0.5850*\dx},{0.0471*\dy}) + -- ({0.5865*\dx},{0.0504*\dy}) + -- ({0.5880*\dx},{0.0536*\dy}) + -- ({0.5896*\dx},{0.0568*\dy}) + -- ({0.5911*\dx},{0.0599*\dy}) + -- ({0.5926*\dx},{0.0631*\dy}) + -- ({0.5942*\dx},{0.0663*\dy}) + -- ({0.5957*\dx},{0.0694*\dy}) + -- ({0.5973*\dx},{0.0725*\dy}) + -- ({0.5988*\dx},{0.0757*\dy}) + -- ({0.6004*\dx},{0.0788*\dy}) + -- ({0.6020*\dx},{0.0819*\dy}) + -- ({0.6036*\dx},{0.0850*\dy}) + -- ({0.6052*\dx},{0.0880*\dy}) + -- ({0.6068*\dx},{0.0911*\dy}) + -- ({0.6084*\dx},{0.0942*\dy}) + -- ({0.6100*\dx},{0.0972*\dy}) + -- ({0.6117*\dx},{0.1002*\dy}) + -- ({0.6133*\dx},{0.1033*\dy}) + -- ({0.6149*\dx},{0.1063*\dy}) + -- ({0.6166*\dx},{0.1093*\dy}) + -- ({0.6183*\dx},{0.1123*\dy}) + -- ({0.6200*\dx},{0.1152*\dy}) + -- ({0.6217*\dx},{0.1182*\dy}) + -- ({0.6234*\dx},{0.1212*\dy}) + -- ({0.6251*\dx},{0.1241*\dy}) + -- ({0.6268*\dx},{0.1271*\dy}) + -- ({0.6285*\dx},{0.1300*\dy}) + -- ({0.6303*\dx},{0.1329*\dy}) + -- ({0.6320*\dx},{0.1358*\dy}) + -- ({0.6338*\dx},{0.1387*\dy}) + -- ({0.6356*\dx},{0.1416*\dy}) + -- ({0.6374*\dx},{0.1445*\dy}) + -- ({0.6392*\dx},{0.1473*\dy}) + -- ({0.6410*\dx},{0.1502*\dy}) + -- ({0.6428*\dx},{0.1530*\dy}) + -- ({0.6446*\dx},{0.1559*\dy}) + -- ({0.6465*\dx},{0.1587*\dy}) + -- ({0.6484*\dx},{0.1615*\dy}) + -- ({0.6502*\dx},{0.1643*\dy}) + -- ({0.6521*\dx},{0.1671*\dy}) + -- ({0.6540*\dx},{0.1699*\dy}) + -- ({0.6560*\dx},{0.1727*\dy}) + -- ({0.6579*\dx},{0.1754*\dy}) + -- ({0.6598*\dx},{0.1782*\dy}) + -- ({0.6618*\dx},{0.1809*\dy}) + -- ({0.6638*\dx},{0.1837*\dy}) + -- ({0.6658*\dx},{0.1864*\dy}) + -- ({0.6678*\dx},{0.1891*\dy}) + -- ({0.6698*\dx},{0.1918*\dy}) + -- ({0.6718*\dx},{0.1945*\dy}) + -- ({0.6738*\dx},{0.1972*\dy}) + -- ({0.6759*\dx},{0.1998*\dy}) + -- ({0.6780*\dx},{0.2025*\dy}) + -- ({0.6801*\dx},{0.2052*\dy}) + -- ({0.6822*\dx},{0.2078*\dy}) + -- ({0.6843*\dx},{0.2104*\dy}) + -- ({0.6864*\dx},{0.2130*\dy}) + -- ({0.6886*\dx},{0.2156*\dy}) + -- ({0.6907*\dx},{0.2182*\dy}) + -- ({0.6929*\dx},{0.2208*\dy}) + -- ({0.6951*\dx},{0.2234*\dy}) + -- ({0.6973*\dx},{0.2260*\dy}) + -- ({0.6996*\dx},{0.2285*\dy}) + -- ({0.7018*\dx},{0.2310*\dy}) + -- ({0.7041*\dx},{0.2336*\dy}) + -- ({0.7064*\dx},{0.2361*\dy}) + -- ({0.7087*\dx},{0.2386*\dy}) + -- ({0.7110*\dx},{0.2411*\dy}) + -- ({0.7133*\dx},{0.2436*\dy}) + -- ({0.7156*\dx},{0.2460*\dy}) + -- ({0.7180*\dx},{0.2485*\dy}) + -- ({0.7204*\dx},{0.2509*\dy}) + -- ({0.7228*\dx},{0.2533*\dy}) + -- ({0.7252*\dx},{0.2558*\dy}) + -- ({0.7276*\dx},{0.2582*\dy}) + -- ({0.7301*\dx},{0.2606*\dy}) + -- ({0.7326*\dx},{0.2629*\dy}) + -- ({0.7350*\dx},{0.2653*\dy}) + -- ({0.7376*\dx},{0.2677*\dy}) + -- ({0.7401*\dx},{0.2700*\dy}) + -- ({0.7426*\dx},{0.2723*\dy}) + -- ({0.7452*\dx},{0.2746*\dy}) + -- ({0.7478*\dx},{0.2769*\dy}) + -- ({0.7504*\dx},{0.2792*\dy}) + -- ({0.7530*\dx},{0.2815*\dy}) + -- ({0.7556*\dx},{0.2837*\dy}) + -- ({0.7583*\dx},{0.2860*\dy}) + -- ({0.7609*\dx},{0.2882*\dy}) + -- ({0.7636*\dx},{0.2904*\dy}) + -- ({0.7663*\dx},{0.2926*\dy}) + -- ({0.7691*\dx},{0.2948*\dy}) + -- ({0.7718*\dx},{0.2969*\dy}) + -- ({0.7746*\dx},{0.2991*\dy}) + -- ({0.7774*\dx},{0.3012*\dy}) + -- ({0.7802*\dx},{0.3033*\dy}) + -- ({0.7830*\dx},{0.3054*\dy}) + -- ({0.7858*\dx},{0.3075*\dy}) + -- ({0.7887*\dx},{0.3096*\dy}) + -- ({0.7916*\dx},{0.3116*\dy}) + -- ({0.7945*\dx},{0.3137*\dy}) + -- ({0.7974*\dx},{0.3157*\dy}) + -- ({0.8004*\dx},{0.3177*\dy}) + -- ({0.8033*\dx},{0.3197*\dy}) + -- ({0.8063*\dx},{0.3216*\dy}) + -- ({0.8093*\dx},{0.3236*\dy}) + -- ({0.8123*\dx},{0.3255*\dy}) + -- ({0.8154*\dx},{0.3274*\dy}) + -- ({0.8184*\dx},{0.3293*\dy}) + -- ({0.8215*\dx},{0.3312*\dy}) + -- ({0.8246*\dx},{0.3330*\dy}) + -- ({0.8277*\dx},{0.3348*\dy}) + -- ({0.8309*\dx},{0.3367*\dy}) + -- ({0.8340*\dx},{0.3384*\dy}) + -- ({0.8372*\dx},{0.3402*\dy}) + -- ({0.8404*\dx},{0.3420*\dy}) + -- ({0.8437*\dx},{0.3437*\dy}) + -- ({0.8469*\dx},{0.3454*\dy}) + -- ({0.8502*\dx},{0.3471*\dy}) + -- ({0.8534*\dx},{0.3487*\dy}) + -- ({0.8567*\dx},{0.3504*\dy}) + -- ({0.8601*\dx},{0.3520*\dy}) + -- ({0.8634*\dx},{0.3536*\dy}) + -- ({0.8668*\dx},{0.3552*\dy}) + -- ({0.8702*\dx},{0.3567*\dy}) + -- ({0.8736*\dx},{0.3583*\dy}) + -- ({0.8770*\dx},{0.3598*\dy}) + -- ({0.8804*\dx},{0.3612*\dy}) + -- ({0.8839*\dx},{0.3627*\dy}) + -- ({0.8874*\dx},{0.3641*\dy}) + -- ({0.8909*\dx},{0.3655*\dy}) + -- ({0.8944*\dx},{0.3669*\dy}) + -- ({0.8980*\dx},{0.3683*\dy}) + -- ({0.9015*\dx},{0.3696*\dy}) + -- ({0.9051*\dx},{0.3709*\dy}) + -- ({0.9087*\dx},{0.3722*\dy}) + -- ({0.9124*\dx},{0.3734*\dy}) + -- ({0.9160*\dx},{0.3746*\dy}) + -- ({0.9197*\dx},{0.3758*\dy}) + -- ({0.9233*\dx},{0.3770*\dy}) + -- ({0.9271*\dx},{0.3781*\dy}) + -- ({0.9308*\dx},{0.3793*\dy}) + -- ({0.9345*\dx},{0.3803*\dy}) + -- ({0.9383*\dx},{0.3814*\dy}) + -- ({0.9421*\dx},{0.3824*\dy}) + -- ({0.9459*\dx},{0.3834*\dy}) + -- ({0.9497*\dx},{0.3844*\dy}) + -- ({0.9535*\dx},{0.3853*\dy}) + -- ({0.9574*\dx},{0.3862*\dy}) + -- ({0.9612*\dx},{0.3871*\dy}) + -- ({0.9651*\dx},{0.3879*\dy}) + -- ({0.9690*\dx},{0.3887*\dy}) + -- ({0.9730*\dx},{0.3895*\dy}) + -- ({0.9769*\dx},{0.3902*\dy}) + -- ({0.9809*\dx},{0.3910*\dy}) + -- ({0.9848*\dx},{0.3916*\dy}) + -- ({0.9888*\dx},{0.3923*\dy}) + -- ({0.9929*\dx},{0.3929*\dy}) + -- ({0.9969*\dx},{0.3935*\dy}) + -- ({1.0009*\dx},{0.3940*\dy}) + -- ({1.0050*\dx},{0.3945*\dy}) + -- ({1.0091*\dx},{0.3950*\dy}) + -- ({1.0132*\dx},{0.3954*\dy}) + -- ({1.0173*\dx},{0.3958*\dy}) + -- ({1.0214*\dx},{0.3962*\dy}) + -- ({1.0256*\dx},{0.3965*\dy}) + -- ({1.0297*\dx},{0.3968*\dy}) + -- ({1.0339*\dx},{0.3971*\dy}) + -- ({1.0381*\dx},{0.3973*\dy}) + -- ({1.0423*\dx},{0.3975*\dy}) + -- ({1.0465*\dx},{0.3976*\dy}) + -- ({1.0508*\dx},{0.3977*\dy}) + -- ({1.0550*\dx},{0.3977*\dy}) + -- ({1.0593*\dx},{0.3978*\dy}) + -- ({1.0636*\dx},{0.3977*\dy}) + -- ({1.0679*\dx},{0.3977*\dy}) + -- ({1.0722*\dx},{0.3976*\dy}) + -- ({1.0765*\dx},{0.3974*\dy}) + -- ({1.0808*\dx},{0.3973*\dy}) + -- ({1.0851*\dx},{0.3970*\dy}) + -- ({1.0895*\dx},{0.3968*\dy}) + -- ({1.0938*\dx},{0.3965*\dy}) + -- ({1.0982*\dx},{0.3961*\dy}) + -- ({1.1026*\dx},{0.3957*\dy}) + -- ({1.1070*\dx},{0.3953*\dy}) + -- ({1.1114*\dx},{0.3948*\dy}) + -- ({1.1158*\dx},{0.3943*\dy}) + -- ({1.1202*\dx},{0.3937*\dy}) + -- ({1.1247*\dx},{0.3931*\dy}) + -- ({1.1291*\dx},{0.3924*\dy}) + -- ({1.1336*\dx},{0.3917*\dy}) + -- ({1.1380*\dx},{0.3909*\dy}) + -- ({1.1425*\dx},{0.3901*\dy}) + -- ({1.1469*\dx},{0.3893*\dy}) + -- ({1.1514*\dx},{0.3884*\dy}) + -- ({1.1559*\dx},{0.3875*\dy}) + -- ({1.1604*\dx},{0.3865*\dy}) + -- ({1.1649*\dx},{0.3854*\dy}) + -- ({1.1694*\dx},{0.3843*\dy}) + -- ({1.1739*\dx},{0.3832*\dy}) + -- ({1.1784*\dx},{0.3820*\dy}) + -- ({1.1829*\dx},{0.3808*\dy}) + -- ({1.1874*\dx},{0.3795*\dy}) + -- ({1.1919*\dx},{0.3782*\dy}) + -- ({1.1965*\dx},{0.3768*\dy}) + -- ({1.2010*\dx},{0.3753*\dy}) + -- ({1.2055*\dx},{0.3738*\dy}) + -- ({1.2100*\dx},{0.3723*\dy}) + -- ({1.2145*\dx},{0.3707*\dy}) + -- ({1.2190*\dx},{0.3691*\dy}) + -- ({1.2236*\dx},{0.3674*\dy}) + -- ({1.2281*\dx},{0.3656*\dy}) + -- ({1.2326*\dx},{0.3638*\dy}) + -- ({1.2371*\dx},{0.3620*\dy}) + -- ({1.2416*\dx},{0.3600*\dy}) + -- ({1.2461*\dx},{0.3581*\dy}) + -- ({1.2506*\dx},{0.3561*\dy}) + -- ({1.2551*\dx},{0.3540*\dy}) + -- ({1.2596*\dx},{0.3519*\dy}) + -- ({1.2641*\dx},{0.3497*\dy}) + -- ({1.2686*\dx},{0.3475*\dy}) + -- ({1.2730*\dx},{0.3452*\dy}) + -- ({1.2775*\dx},{0.3428*\dy}) + -- ({1.2819*\dx},{0.3404*\dy}) + -- ({1.2864*\dx},{0.3379*\dy}) + -- ({1.2908*\dx},{0.3354*\dy}) + -- ({1.2952*\dx},{0.3329*\dy}) + -- ({1.2996*\dx},{0.3302*\dy}) + -- ({1.3040*\dx},{0.3275*\dy}) + -- ({1.3084*\dx},{0.3248*\dy}) + -- ({1.3128*\dx},{0.3220*\dy}) + -- ({1.3171*\dx},{0.3191*\dy}) + -- ({1.3215*\dx},{0.3162*\dy}) + -- ({1.3258*\dx},{0.3132*\dy}) + -- ({1.3301*\dx},{0.3102*\dy}) + -- ({1.3344*\dx},{0.3071*\dy}) + -- ({1.3386*\dx},{0.3040*\dy}) + -- ({1.3429*\dx},{0.3008*\dy}) + -- ({1.3471*\dx},{0.2975*\dy}) + -- ({1.3513*\dx},{0.2942*\dy}) + -- ({1.3555*\dx},{0.2908*\dy}) + -- ({1.3597*\dx},{0.2874*\dy}) + -- ({1.3638*\dx},{0.2839*\dy}) + -- ({1.3680*\dx},{0.2803*\dy}) + -- ({1.3721*\dx},{0.2767*\dy}) + -- ({1.3761*\dx},{0.2730*\dy}) + -- ({1.3802*\dx},{0.2693*\dy}) + -- ({1.3842*\dx},{0.2655*\dy}) + -- ({1.3882*\dx},{0.2616*\dy}) + -- ({1.3922*\dx},{0.2577*\dy}) + -- ({1.3961*\dx},{0.2537*\dy}) + -- ({1.4000*\dx},{0.2497*\dy}) + -- ({1.4039*\dx},{0.2456*\dy}) + -- ({1.4077*\dx},{0.2414*\dy}) + -- ({1.4115*\dx},{0.2372*\dy}) + -- ({1.4153*\dx},{0.2329*\dy}) + -- ({1.4191*\dx},{0.2286*\dy}) + -- ({1.4228*\dx},{0.2242*\dy}) + -- ({1.4264*\dx},{0.2197*\dy}) + -- ({1.4301*\dx},{0.2152*\dy}) + -- ({1.4337*\dx},{0.2107*\dy}) + -- ({1.4372*\dx},{0.2060*\dy}) + -- ({1.4407*\dx},{0.2014*\dy}) + -- ({1.4442*\dx},{0.1966*\dy}) + -- ({1.4476*\dx},{0.1918*\dy}) + -- ({1.4510*\dx},{0.1869*\dy}) + -- ({1.4544*\dx},{0.1820*\dy}) + -- ({1.4577*\dx},{0.1770*\dy}) + -- ({1.4609*\dx},{0.1720*\dy}) + -- ({1.4642*\dx},{0.1669*\dy}) + -- ({1.4673*\dx},{0.1618*\dy}) + -- ({1.4704*\dx},{0.1566*\dy}) + -- ({1.4735*\dx},{0.1513*\dy}) + -- ({1.4765*\dx},{0.1460*\dy}) + -- ({1.4795*\dx},{0.1406*\dy}) + -- ({1.4824*\dx},{0.1352*\dy}) + -- ({1.4853*\dx},{0.1297*\dy}) + -- ({1.4881*\dx},{0.1241*\dy}) + -- ({1.4908*\dx},{0.1185*\dy}) + -- ({1.4935*\dx},{0.1129*\dy}) + -- ({1.4961*\dx},{0.1072*\dy}) + -- ({1.4987*\dx},{0.1014*\dy}) + -- ({1.5012*\dx},{0.0956*\dy}) + -- ({1.5037*\dx},{0.0897*\dy}) + -- ({1.5061*\dx},{0.0838*\dy}) + -- ({1.5084*\dx},{0.0778*\dy}) + -- ({1.5107*\dx},{0.0718*\dy}) + -- ({1.5129*\dx},{0.0657*\dy}) + -- ({1.5151*\dx},{0.0596*\dy}) + -- ({1.5172*\dx},{0.0534*\dy}) + -- ({1.5192*\dx},{0.0472*\dy}) + -- ({1.5211*\dx},{0.0409*\dy}) + -- ({1.5230*\dx},{0.0346*\dy}) + -- ({1.5248*\dx},{0.0282*\dy}) + -- ({1.5265*\dx},{0.0218*\dy}) + -- ({1.5282*\dx},{0.0153*\dy}) + -- ({1.5298*\dx},{0.0088*\dy}) + -- ({1.5313*\dx},{0.0023*\dy}) + -- ({1.5328*\dx},{-0.0043*\dy}) + -- ({1.5341*\dx},{-0.0110*\dy}) + -- ({1.5354*\dx},{-0.0177*\dy}) + -- ({1.5366*\dx},{-0.0244*\dy}) + -- ({1.5378*\dx},{-0.0312*\dy}) + -- ({1.5388*\dx},{-0.0380*\dy}) + -- ({1.5398*\dx},{-0.0448*\dy}) + -- ({1.5407*\dx},{-0.0517*\dy}) + -- ({1.5415*\dx},{-0.0586*\dy}) + -- ({1.5422*\dx},{-0.0656*\dy}) + -- ({1.5429*\dx},{-0.0726*\dy}) + -- ({1.5434*\dx},{-0.0796*\dy}) + -- ({1.5439*\dx},{-0.0867*\dy}) + -- ({1.5443*\dx},{-0.0938*\dy}) + -- ({1.5446*\dx},{-0.1010*\dy}) + -- ({1.5448*\dx},{-0.1081*\dy}) + -- ({1.5449*\dx},{-0.1153*\dy}) + -- ({1.5449*\dx},{-0.1226*\dy}) + -- ({1.5449*\dx},{-0.1298*\dy}) + -- ({1.5447*\dx},{-0.1371*\dy}) + -- ({1.5444*\dx},{-0.1444*\dy}) + -- ({1.5441*\dx},{-0.1518*\dy}) + -- ({1.5437*\dx},{-0.1591*\dy}) + -- ({1.5431*\dx},{-0.1665*\dy}) + -- ({1.5425*\dx},{-0.1740*\dy}) + -- ({1.5418*\dx},{-0.1814*\dy}) + -- ({1.5409*\dx},{-0.1888*\dy}) + -- ({1.5400*\dx},{-0.1963*\dy}) + -- ({1.5390*\dx},{-0.2038*\dy}) + -- ({1.5378*\dx},{-0.2113*\dy}) + -- ({1.5366*\dx},{-0.2188*\dy}) + -- ({1.5353*\dx},{-0.2264*\dy}) + -- ({1.5339*\dx},{-0.2339*\dy}) + -- ({1.5323*\dx},{-0.2415*\dy}) + -- ({1.5307*\dx},{-0.2491*\dy}) + -- ({1.5289*\dx},{-0.2566*\dy}) + -- ({1.5271*\dx},{-0.2642*\dy}) + -- ({1.5251*\dx},{-0.2718*\dy}) + -- ({1.5230*\dx},{-0.2794*\dy}) + -- ({1.5209*\dx},{-0.2870*\dy}) + -- ({1.5186*\dx},{-0.2946*\dy}) + -- ({1.5162*\dx},{-0.3022*\dy}) + -- ({1.5137*\dx},{-0.3098*\dy}) + -- ({1.5111*\dx},{-0.3174*\dy}) + -- ({1.5084*\dx},{-0.3250*\dy}) + -- ({1.5055*\dx},{-0.3326*\dy}) + -- ({1.5026*\dx},{-0.3402*\dy}) + -- ({1.4995*\dx},{-0.3477*\dy}) + -- ({1.4963*\dx},{-0.3553*\dy}) + -- ({1.4931*\dx},{-0.3628*\dy}) + -- ({1.4897*\dx},{-0.3704*\dy}) + -- ({1.4862*\dx},{-0.3779*\dy}) + -- ({1.4825*\dx},{-0.3854*\dy}) + -- ({1.4788*\dx},{-0.3929*\dy}) + -- ({1.4749*\dx},{-0.4003*\dy}) + -- ({1.4710*\dx},{-0.4078*\dy}) + -- ({1.4669*\dx},{-0.4152*\dy}) + -- ({1.4627*\dx},{-0.4226*\dy}) + -- ({1.4584*\dx},{-0.4300*\dy}) + -- ({1.4539*\dx},{-0.4373*\dy}) + -- ({1.4494*\dx},{-0.4446*\dy}) + -- ({1.4447*\dx},{-0.4519*\dy}) + -- ({1.4399*\dx},{-0.4591*\dy}) + -- ({1.4350*\dx},{-0.4663*\dy}) + -- ({1.4300*\dx},{-0.4735*\dy}) + -- ({1.4249*\dx},{-0.4806*\dy}) + -- ({1.4197*\dx},{-0.4877*\dy}) + -- ({1.4143*\dx},{-0.4947*\dy}) + -- ({1.4088*\dx},{-0.5017*\dy}) + -- ({1.4032*\dx},{-0.5086*\dy}) + -- ({1.3975*\dx},{-0.5155*\dy}) + -- ({1.3916*\dx},{-0.5224*\dy}) + -- ({1.3857*\dx},{-0.5292*\dy}) + -- ({1.3796*\dx},{-0.5359*\dy}) + -- ({1.3734*\dx},{-0.5426*\dy}) + -- ({1.3671*\dx},{-0.5492*\dy}) + -- ({1.3607*\dx},{-0.5558*\dy}) + -- ({1.3542*\dx},{-0.5623*\dy}) + -- ({1.3475*\dx},{-0.5687*\dy}) + -- ({1.3408*\dx},{-0.5751*\dy}) + -- ({1.3339*\dx},{-0.5814*\dy}) + -- ({1.3269*\dx},{-0.5876*\dy}) + -- ({1.3198*\dx},{-0.5937*\dy}) + -- ({1.3126*\dx},{-0.5998*\dy}) + -- ({1.3052*\dx},{-0.6058*\dy}) + -- ({1.2978*\dx},{-0.6117*\dy}) + -- ({1.2902*\dx},{-0.6176*\dy}) + -- ({1.2826*\dx},{-0.6233*\dy}) + -- ({1.2748*\dx},{-0.6290*\dy}) + -- ({1.2669*\dx},{-0.6346*\dy}) + -- ({1.2589*\dx},{-0.6401*\dy}) + -- ({1.2508*\dx},{-0.6455*\dy}) + -- ({1.2426*\dx},{-0.6508*\dy}) + -- ({1.2343*\dx},{-0.6560*\dy}) + -- ({1.2259*\dx},{-0.6611*\dy}) + -- ({1.2173*\dx},{-0.6662*\dy}) + -- ({1.2087*\dx},{-0.6711*\dy}) + -- ({1.2000*\dx},{-0.6759*\dy}) + -- ({1.1911*\dx},{-0.6806*\dy}) + -- ({1.1822*\dx},{-0.6852*\dy}) + -- ({1.1731*\dx},{-0.6897*\dy}) + -- ({1.1640*\dx},{-0.6941*\dy}) + -- ({1.1548*\dx},{-0.6984*\dy}) + -- ({1.1454*\dx},{-0.7025*\dy}) + -- ({1.1360*\dx},{-0.7065*\dy}) + -- ({1.1265*\dx},{-0.7105*\dy}) + -- ({1.1169*\dx},{-0.7143*\dy}) + -- ({1.1072*\dx},{-0.7179*\dy}) + -- ({1.0974*\dx},{-0.7215*\dy}) + -- ({1.0875*\dx},{-0.7249*\dy}) + -- ({1.0775*\dx},{-0.7282*\dy}) + -- ({1.0674*\dx},{-0.7313*\dy}) + -- ({1.0573*\dx},{-0.7344*\dy}) + -- ({1.0471*\dx},{-0.7373*\dy}) + -- ({1.0368*\dx},{-0.7400*\dy}) + -- ({1.0264*\dx},{-0.7426*\dy}) + -- ({1.0159*\dx},{-0.7451*\dy}) + -- ({1.0054*\dx},{-0.7474*\dy}) + -- ({0.9948*\dx},{-0.7496*\dy}) + -- ({0.9841*\dx},{-0.7517*\dy}) + -- ({0.9734*\dx},{-0.7536*\dy}) + -- ({0.9625*\dx},{-0.7553*\dy}) + -- ({0.9516*\dx},{-0.7569*\dy}) + -- ({0.9407*\dx},{-0.7584*\dy}) + -- ({0.9297*\dx},{-0.7596*\dy}) + -- ({0.9186*\dx},{-0.7608*\dy}) + -- ({0.9075*\dx},{-0.7617*\dy}) + -- ({0.8963*\dx},{-0.7626*\dy}) + -- ({0.8850*\dx},{-0.7632*\dy}) + -- ({0.8738*\dx},{-0.7637*\dy}) + -- ({0.8624*\dx},{-0.7640*\dy}) + -- ({0.8510*\dx},{-0.7642*\dy}) + -- ({0.8396*\dx},{-0.7642*\dy}) + -- ({0.8281*\dx},{-0.7640*\dy}) + -- ({0.8166*\dx},{-0.7636*\dy}) + -- ({0.8050*\dx},{-0.7631*\dy}) + -- ({0.7934*\dx},{-0.7624*\dy}) + -- ({0.7818*\dx},{-0.7615*\dy}) + -- ({0.7702*\dx},{-0.7605*\dy}) + -- ({0.7585*\dx},{-0.7593*\dy}) + -- ({0.7468*\dx},{-0.7579*\dy}) + -- ({0.7350*\dx},{-0.7563*\dy}) + -- ({0.7233*\dx},{-0.7545*\dy}) + -- ({0.7115*\dx},{-0.7526*\dy}) + -- ({0.6998*\dx},{-0.7504*\dy}) + -- ({0.6880*\dx},{-0.7481*\dy}) + -- ({0.6762*\dx},{-0.7456*\dy}) + -- ({0.6644*\dx},{-0.7429*\dy}) + -- ({0.6526*\dx},{-0.7401*\dy}) + -- ({0.6407*\dx},{-0.7370*\dy}) + -- ({0.6289*\dx},{-0.7337*\dy}) + -- ({0.6171*\dx},{-0.7303*\dy}) + -- ({0.6054*\dx},{-0.7267*\dy}) + -- ({0.5936*\dx},{-0.7229*\dy}) + -- ({0.5818*\dx},{-0.7188*\dy}) + -- ({0.5701*\dx},{-0.7146*\dy}) + -- ({0.5583*\dx},{-0.7102*\dy}) + -- ({0.5466*\dx},{-0.7056*\dy}) + -- ({0.5350*\dx},{-0.7008*\dy}) + -- ({0.5233*\dx},{-0.6959*\dy}) + -- ({0.5117*\dx},{-0.6907*\dy}) + -- ({0.5002*\dx},{-0.6853*\dy}) + -- ({0.4886*\dx},{-0.6797*\dy}) + -- ({0.4772*\dx},{-0.6740*\dy}) + -- ({0.4657*\dx},{-0.6680*\dy}) + -- ({0.4543*\dx},{-0.6618*\dy}) + -- ({0.4430*\dx},{-0.6555*\dy}) + -- ({0.4317*\dx},{-0.6489*\dy}) + -- ({0.4205*\dx},{-0.6422*\dy}) + -- ({0.4094*\dx},{-0.6352*\dy}) + -- ({0.3983*\dx},{-0.6281*\dy}) + -- ({0.3873*\dx},{-0.6208*\dy}) + -- ({0.3763*\dx},{-0.6132*\dy}) + -- ({0.3655*\dx},{-0.6055*\dy}) + -- ({0.3547*\dx},{-0.5976*\dy}) + -- ({0.3440*\dx},{-0.5894*\dy}) + -- ({0.3334*\dx},{-0.5811*\dy}) + -- ({0.3229*\dx},{-0.5726*\dy}) + -- ({0.3125*\dx},{-0.5639*\dy}) + -- ({0.3022*\dx},{-0.5550*\dy}) + -- ({0.2920*\dx},{-0.5459*\dy}) + -- ({0.2818*\dx},{-0.5367*\dy}) + -- ({0.2718*\dx},{-0.5272*\dy}) + -- ({0.2620*\dx},{-0.5175*\dy}) + -- ({0.2522*\dx},{-0.5077*\dy}) + -- ({0.2425*\dx},{-0.4977*\dy}) + -- ({0.2330*\dx},{-0.4875*\dy}) + -- ({0.2236*\dx},{-0.4771*\dy}) + -- ({0.2144*\dx},{-0.4665*\dy}) + -- ({0.2052*\dx},{-0.4557*\dy}) + -- ({0.1962*\dx},{-0.4448*\dy}) + -- ({0.1874*\dx},{-0.4337*\dy}) + -- ({0.1787*\dx},{-0.4224*\dy}) + -- ({0.1701*\dx},{-0.4109*\dy}) + -- ({0.1617*\dx},{-0.3992*\dy}) + -- ({0.1535*\dx},{-0.3874*\dy}) + -- ({0.1454*\dx},{-0.3754*\dy}) + -- ({0.1375*\dx},{-0.3633*\dy}) + -- ({0.1297*\dx},{-0.3509*\dy}) + -- ({0.1221*\dx},{-0.3384*\dy}) + -- ({0.1147*\dx},{-0.3258*\dy}) + -- ({0.1074*\dx},{-0.3130*\dy}) + -- ({0.1004*\dx},{-0.3000*\dy}) + -- ({0.0935*\dx},{-0.2869*\dy}) + -- ({0.0868*\dx},{-0.2736*\dy}) + -- ({0.0803*\dx},{-0.2602*\dy}) + -- ({0.0740*\dx},{-0.2466*\dy}) + -- ({0.0679*\dx},{-0.2329*\dy}) + -- ({0.0620*\dx},{-0.2190*\dy}) + -- ({0.0563*\dx},{-0.2050*\dy}) + -- ({0.0508*\dx},{-0.1908*\dy}) + -- ({0.0455*\dx},{-0.1766*\dy}) + -- ({0.0404*\dx},{-0.1622*\dy}) + -- ({0.0355*\dx},{-0.1476*\dy}) + -- ({0.0309*\dx},{-0.1330*\dy}) + -- ({0.0264*\dx},{-0.1182*\dy}) + -- ({0.0222*\dx},{-0.1033*\dy}) + -- ({0.0183*\dx},{-0.0882*\dy}) + -- ({0.0145*\dx},{-0.0731*\dy}) + -- ({0.0110*\dx},{-0.0579*\dy}) + -- ({0.0077*\dx},{-0.0425*\dy}) + -- ({0.0047*\dx},{-0.0271*\dy}) + -- ({0.0019*\dx},{-0.0115*\dy}) + -- ({-0.0006*\dx},{0.0041*\dy}) + -- ({-0.0030*\dx},{0.0199*\dy}) + -- ({-0.0050*\dx},{0.0357*\dy}) + -- ({-0.0068*\dx},{0.0516*\dy}) + -- ({-0.0084*\dx},{0.0676*\dy}) + -- ({-0.0097*\dx},{0.0836*\dy}) + -- ({-0.0107*\dx},{0.0998*\dy}) + -- ({-0.0115*\dx},{0.1160*\dy}) + -- ({-0.0120*\dx},{0.1322*\dy}) + -- ({-0.0122*\dx},{0.1486*\dy}) + -- ({-0.0122*\dx},{0.1649*\dy}) + -- ({-0.0119*\dx},{0.1813*\dy}) + -- ({-0.0114*\dx},{0.1978*\dy}) + -- ({-0.0105*\dx},{0.2143*\dy}) + -- ({-0.0094*\dx},{0.2309*\dy}) + -- ({-0.0080*\dx},{0.2475*\dy}) + -- ({-0.0064*\dx},{0.2641*\dy}) + -- ({-0.0044*\dx},{0.2807*\dy}) + -- ({-0.0022*\dx},{0.2973*\dy}) + -- ({0.0003*\dx},{0.3140*\dy}) + -- ({0.0031*\dx},{0.3307*\dy}) + -- ({0.0061*\dx},{0.3473*\dy}) + -- ({0.0095*\dx},{0.3640*\dy}) + -- ({0.0131*\dx},{0.3807*\dy}) + -- ({0.0171*\dx},{0.3973*\dy}) + -- ({0.0213*\dx},{0.4140*\dy}) + -- ({0.0258*\dx},{0.4306*\dy}) + -- ({0.0306*\dx},{0.4472*\dy}) + -- ({0.0357*\dx},{0.4637*\dy}) + -- ({0.0411*\dx},{0.4803*\dy}) + -- ({0.0467*\dx},{0.4967*\dy}) + -- ({0.0527*\dx},{0.5132*\dy}) + -- ({0.0590*\dx},{0.5296*\dy}) + -- ({0.0655*\dx},{0.5459*\dy}) + -- ({0.0724*\dx},{0.5621*\dy}) + -- ({0.0795*\dx},{0.5783*\dy}) + -- ({0.0869*\dx},{0.5945*\dy}) + -- ({0.0947*\dx},{0.6105*\dy}) + -- ({0.1027*\dx},{0.6264*\dy}) + -- ({0.1110*\dx},{0.6423*\dy}) + -- ({0.1196*\dx},{0.6581*\dy}) + -- ({0.1285*\dx},{0.6737*\dy}) + -- ({0.1376*\dx},{0.6893*\dy}) + -- ({0.1471*\dx},{0.7048*\dy}) + -- ({0.1569*\dx},{0.7201*\dy}) + -- ({0.1669*\dx},{0.7353*\dy}) + -- ({0.1772*\dx},{0.7504*\dy}) + -- ({0.1878*\dx},{0.7653*\dy}) + -- ({0.1987*\dx},{0.7801*\dy}) + -- ({0.2099*\dx},{0.7948*\dy}) + -- ({0.2214*\dx},{0.8093*\dy}) + -- ({0.2331*\dx},{0.8236*\dy}) + -- ({0.2451*\dx},{0.8378*\dy}) + -- ({0.2574*\dx},{0.8519*\dy}) + -- ({0.2700*\dx},{0.8657*\dy}) + -- ({0.2828*\dx},{0.8794*\dy}) + -- ({0.2959*\dx},{0.8929*\dy}) + -- ({0.3093*\dx},{0.9062*\dy}) + -- ({0.3229*\dx},{0.9193*\dy}) + -- ({0.3368*\dx},{0.9322*\dy}) + -- ({0.3509*\dx},{0.9449*\dy}) + -- ({0.3653*\dx},{0.9574*\dy}) + -- ({0.3800*\dx},{0.9697*\dy}) + -- ({0.3949*\dx},{0.9817*\dy}) + -- ({0.4100*\dx},{0.9936*\dy}) + -- ({0.4254*\dx},{1.0052*\dy}) + -- ({0.4411*\dx},{1.0165*\dy}) + -- ({0.4569*\dx},{1.0276*\dy}) + -- ({0.4730*\dx},{1.0385*\dy}) + -- ({0.4894*\dx},{1.0491*\dy}) + -- ({0.5059*\dx},{1.0595*\dy}) + -- ({0.5227*\dx},{1.0696*\dy}) + -- ({0.5397*\dx},{1.0795*\dy}) + -- ({0.5569*\dx},{1.0890*\dy}) + -- ({0.5743*\dx},{1.0983*\dy}) + -- ({0.5919*\dx},{1.1073*\dy}) + -- ({0.6098*\dx},{1.1160*\dy}) + -- ({0.6278*\dx},{1.1245*\dy}) + -- ({0.6460*\dx},{1.1326*\dy}) + -- ({0.6644*\dx},{1.1405*\dy}) + -- ({0.6830*\dx},{1.1480*\dy}) + -- ({0.7017*\dx},{1.1552*\dy}) + -- ({0.7206*\dx},{1.1622*\dy}) + -- ({0.7397*\dx},{1.1688*\dy}) + -- ({0.7590*\dx},{1.1750*\dy}) + -- ({0.7784*\dx},{1.1810*\dy}) + -- ({0.7979*\dx},{1.1866*\dy}) + -- ({0.8176*\dx},{1.1919*\dy}) + -- ({0.8375*\dx},{1.1969*\dy}) + -- ({0.8574*\dx},{1.2015*\dy}) + -- ({0.8775*\dx},{1.2058*\dy}) + -- ({0.8978*\dx},{1.2098*\dy}) + -- ({0.9181*\dx},{1.2133*\dy}) + -- ({0.9385*\dx},{1.2166*\dy}) + -- ({0.9591*\dx},{1.2195*\dy}) + -- ({0.9797*\dx},{1.2220*\dy}) + -- ({1.0005*\dx},{1.2242*\dy}) + -- ({1.0213*\dx},{1.2260*\dy}) + -- ({1.0422*\dx},{1.2274*\dy}) + -- ({1.0632*\dx},{1.2285*\dy}) + -- ({1.0842*\dx},{1.2292*\dy}) + -- ({1.1053*\dx},{1.2295*\dy}) + -- ({1.1264*\dx},{1.2294*\dy}) + -- ({1.1476*\dx},{1.2290*\dy}) + -- ({1.1688*\dx},{1.2282*\dy}) + -- ({1.1901*\dx},{1.2270*\dy}) + -- ({1.2114*\dx},{1.2254*\dy}) + -- ({1.2327*\dx},{1.2234*\dy}) + -- ({1.2540*\dx},{1.2211*\dy}) + -- ({1.2753*\dx},{1.2184*\dy}) + -- ({1.2965*\dx},{1.2152*\dy}) + -- ({1.3178*\dx},{1.2117*\dy}) + -- ({1.3391*\dx},{1.2078*\dy}) + -- ({1.3603*\dx},{1.2035*\dy}) + -- ({1.3815*\dx},{1.1988*\dy}) + -- ({1.4027*\dx},{1.1938*\dy}) + -- ({1.4238*\dx},{1.1883*\dy}) + -- ({1.4448*\dx},{1.1824*\dy}) + -- ({1.4658*\dx},{1.1762*\dy}) + -- ({1.4867*\dx},{1.1695*\dy}) + -- ({1.5076*\dx},{1.1625*\dy}) + -- ({1.5283*\dx},{1.1550*\dy}) + -- ({1.5489*\dx},{1.1472*\dy}) + -- ({1.5695*\dx},{1.1390*\dy}) + -- ({1.5899*\dx},{1.1304*\dy}) + -- ({1.6102*\dx},{1.1214*\dy}) + -- ({1.6304*\dx},{1.1120*\dy}) + -- ({1.6504*\dx},{1.1023*\dy}) + -- ({1.6703*\dx},{1.0921*\dy}) + -- ({1.6901*\dx},{1.0816*\dy}) + -- ({1.7097*\dx},{1.0707*\dy}) + -- ({1.7291*\dx},{1.0594*\dy}) + -- ({1.7484*\dx},{1.0477*\dy}) + -- ({1.7675*\dx},{1.0357*\dy}) + -- ({1.7864*\dx},{1.0233*\dy}) + -- ({1.8051*\dx},{1.0105*\dy}) + -- ({1.8235*\dx},{0.9974*\dy}) + -- ({1.8418*\dx},{0.9839*\dy}) + -- ({1.8599*\dx},{0.9700*\dy}) + -- ({1.8777*\dx},{0.9558*\dy}) + -- ({1.8953*\dx},{0.9412*\dy}) + -- ({1.9127*\dx},{0.9263*\dy}) + -- ({1.9298*\dx},{0.9110*\dy}) + -- ({1.9467*\dx},{0.8954*\dy}) + -- ({1.9632*\dx},{0.8795*\dy}) + -- ({1.9796*\dx},{0.8632*\dy}) + -- ({1.9956*\dx},{0.8466*\dy}) + -- ({2.0114*\dx},{0.8296*\dy}) + -- ({2.0269*\dx},{0.8124*\dy}) + -- ({2.0420*\dx},{0.7948*\dy}) + -- ({2.0569*\dx},{0.7770*\dy}) + -- ({2.0715*\dx},{0.7588*\dy}) + -- ({2.0857*\dx},{0.7403*\dy}) + -- ({2.0996*\dx},{0.7215*\dy}) + -- ({2.1132*\dx},{0.7025*\dy}) + -- ({2.1264*\dx},{0.6831*\dy}) + -- ({2.1393*\dx},{0.6635*\dy}) + -- ({2.1519*\dx},{0.6437*\dy}) + -- ({2.1641*\dx},{0.6235*\dy}) + -- ({2.1759*\dx},{0.6031*\dy}) + -- ({2.1874*\dx},{0.5825*\dy}) + -- ({2.1985*\dx},{0.5616*\dy}) + -- ({2.2092*\dx},{0.5404*\dy}) + -- ({2.2195*\dx},{0.5191*\dy}) + -- ({2.2295*\dx},{0.4975*\dy}) + -- ({2.2390*\dx},{0.4757*\dy}) + -- ({2.2481*\dx},{0.4537*\dy}) + -- ({2.2569*\dx},{0.4315*\dy}) + -- ({2.2652*\dx},{0.4091*\dy}) + -- ({2.2731*\dx},{0.3865*\dy}) + -- ({2.2806*\dx},{0.3638*\dy}) + -- ({2.2877*\dx},{0.3408*\dy}) + -- ({2.2943*\dx},{0.3177*\dy}) + -- ({2.3005*\dx},{0.2945*\dy}) + -- ({2.3063*\dx},{0.2711*\dy}) + -- ({2.3116*\dx},{0.2476*\dy}) + -- ({2.3165*\dx},{0.2239*\dy}) + -- ({2.3210*\dx},{0.2002*\dy}) + -- ({2.3249*\dx},{0.1763*\dy}) + -- ({2.3285*\dx},{0.1523*\dy}) + -- ({2.3316*\dx},{0.1283*\dy}) + -- ({2.3342*\dx},{0.1041*\dy}) + -- ({2.3364*\dx},{0.0799*\dy}) + -- ({2.3381*\dx},{0.0556*\dy}) + -- ({2.3393*\dx},{0.0312*\dy}) + -- ({2.3401*\dx},{0.0068*\dy}) + -- ({2.3403*\dx},{-0.0176*\dy}) + -- ({2.3402*\dx},{-0.0421*\dy}) + -- ({2.3395*\dx},{-0.0665*\dy}) + -- ({2.3384*\dx},{-0.0910*\dy}) + -- ({2.3368*\dx},{-0.1155*\dy}) + -- ({2.3347*\dx},{-0.1400*\dy}) + -- ({2.3322*\dx},{-0.1644*\dy}) + -- ({2.3292*\dx},{-0.1889*\dy}) + -- ({2.3257*\dx},{-0.2133*\dy}) + -- ({2.3217*\dx},{-0.2376*\dy}) + -- ({2.3172*\dx},{-0.2619*\dy}) + -- ({2.3123*\dx},{-0.2861*\dy}) + -- ({2.3069*\dx},{-0.3102*\dy}) + -- ({2.3010*\dx},{-0.3342*\dy}) + -- ({2.2946*\dx},{-0.3582*\dy}) + -- ({2.2878*\dx},{-0.3820*\dy}) + -- ({2.2805*\dx},{-0.4057*\dy}) + -- ({2.2727*\dx},{-0.4293*\dy}) + -- ({2.2645*\dx},{-0.4528*\dy}) + -- ({2.2558*\dx},{-0.4761*\dy}) + -- ({2.2466*\dx},{-0.4992*\dy}) + -- ({2.2370*\dx},{-0.5222*\dy}) + -- ({2.2269*\dx},{-0.5450*\dy}) + -- ({2.2164*\dx},{-0.5676*\dy}) + -- ({2.2054*\dx},{-0.5900*\dy}) + -- ({2.1939*\dx},{-0.6122*\dy}) + -- ({2.1820*\dx},{-0.6342*\dy}) + -- ({2.1697*\dx},{-0.6560*\dy}) + -- ({2.1569*\dx},{-0.6775*\dy}) + -- ({2.1437*\dx},{-0.6988*\dy}) + -- ({2.1301*\dx},{-0.7198*\dy}) + -- ({2.1161*\dx},{-0.7406*\dy}) + -- ({2.1016*\dx},{-0.7611*\dy}) + -- ({2.0867*\dx},{-0.7813*\dy}) + -- ({2.0714*\dx},{-0.8012*\dy}) + -- ({2.0558*\dx},{-0.8208*\dy}) + -- ({2.0397*\dx},{-0.8401*\dy}) + -- ({2.0232*\dx},{-0.8591*\dy}) + -- ({2.0063*\dx},{-0.8778*\dy}) + -- ({1.9891*\dx},{-0.8961*\dy}) + -- ({1.9715*\dx},{-0.9141*\dy}) + -- ({1.9535*\dx},{-0.9318*\dy}) + -- ({1.9352*\dx},{-0.9491*\dy}) + -- ({1.9165*\dx},{-0.9660*\dy}) + -- ({1.8974*\dx},{-0.9825*\dy}) + -- ({1.8781*\dx},{-0.9987*\dy}) + -- ({1.8584*\dx},{-1.0144*\dy}) + -- ({1.8384*\dx},{-1.0298*\dy}) + -- ({1.8181*\dx},{-1.0448*\dy}) + -- ({1.7974*\dx},{-1.0593*\dy}) + -- ({1.7765*\dx},{-1.0735*\dy}) + -- ({1.7553*\dx},{-1.0872*\dy}) + -- ({1.7338*\dx},{-1.1004*\dy}) + -- ({1.7120*\dx},{-1.1133*\dy}) + -- ({1.6900*\dx},{-1.1257*\dy}) + -- ({1.6677*\dx},{-1.1376*\dy}) + -- ({1.6452*\dx},{-1.1491*\dy}) + -- ({1.6225*\dx},{-1.1601*\dy}) + -- ({1.5995*\dx},{-1.1707*\dy}) + -- ({1.5764*\dx},{-1.1808*\dy}) + -- ({1.5530*\dx},{-1.1904*\dy}) + -- ({1.5294*\dx},{-1.1995*\dy}) + -- ({1.5057*\dx},{-1.2081*\dy}) + -- ({1.4817*\dx},{-1.2162*\dy}) + -- ({1.4576*\dx},{-1.2239*\dy}) + -- ({1.4334*\dx},{-1.2310*\dy}) + -- ({1.4090*\dx},{-1.2377*\dy}) + -- ({1.3845*\dx},{-1.2438*\dy}) + -- ({1.3599*\dx},{-1.2494*\dy}) + -- ({1.3352*\dx},{-1.2545*\dy}) + -- ({1.3103*\dx},{-1.2591*\dy}) + -- ({1.2854*\dx},{-1.2632*\dy}) + -- ({1.2605*\dx},{-1.2667*\dy}) + -- ({1.2354*\dx},{-1.2698*\dy}) + -- ({1.2103*\dx},{-1.2723*\dy}) + -- ({1.1852*\dx},{-1.2742*\dy}) + -- ({1.1600*\dx},{-1.2757*\dy}) + -- ({1.1348*\dx},{-1.2766*\dy}) + -- ({1.1097*\dx},{-1.2770*\dy}) + -- ({1.0845*\dx},{-1.2768*\dy}) + -- ({1.0593*\dx},{-1.2762*\dy}) + -- ({1.0342*\dx},{-1.2750*\dy}) + -- ({1.0091*\dx},{-1.2732*\dy}) + -- ({0.9841*\dx},{-1.2710*\dy}) + -- ({0.9591*\dx},{-1.2682*\dy}) + -- ({0.9342*\dx},{-1.2649*\dy}) + -- ({0.9094*\dx},{-1.2610*\dy}) + -- ({0.8848*\dx},{-1.2567*\dy}) + -- ({0.8602*\dx},{-1.2518*\dy}) + -- ({0.8357*\dx},{-1.2464*\dy}) + -- ({0.8114*\dx},{-1.2404*\dy}) + -- ({0.7872*\dx},{-1.2340*\dy}) + -- ({0.7632*\dx},{-1.2271*\dy}) + -- ({0.7394*\dx},{-1.2196*\dy}) + -- ({0.7157*\dx},{-1.2116*\dy}) + -- ({0.6923*\dx},{-1.2032*\dy}) + -- ({0.6690*\dx},{-1.1942*\dy}) + -- ({0.6460*\dx},{-1.1847*\dy}) + -- ({0.6231*\dx},{-1.1748*\dy}) + -- ({0.6006*\dx},{-1.1644*\dy}) + -- ({0.5783*\dx},{-1.1535*\dy}) + -- ({0.5562*\dx},{-1.1421*\dy}) + -- ({0.5344*\dx},{-1.1303*\dy}) + -- ({0.5129*\dx},{-1.1180*\dy}) + -- ({0.4917*\dx},{-1.1052*\dy}) + -- ({0.4708*\dx},{-1.0920*\dy}) + -- ({0.4502*\dx},{-1.0784*\dy}) + -- ({0.4299*\dx},{-1.0643*\dy}) + -- ({0.4100*\dx},{-1.0498*\dy}) + -- ({0.3904*\dx},{-1.0349*\dy}) + -- ({0.3711*\dx},{-1.0195*\dy}) + -- ({0.3523*\dx},{-1.0038*\dy}) + -- ({0.3338*\dx},{-0.9877*\dy}) + -- ({0.3157*\dx},{-0.9712*\dy}) + -- ({0.2979*\dx},{-0.9543*\dy}) + -- ({0.2806*\dx},{-0.9370*\dy}) + -- ({0.2637*\dx},{-0.9194*\dy}) + -- ({0.2472*\dx},{-0.9014*\dy}) + -- ({0.2311*\dx},{-0.8831*\dy}) + -- ({0.2154*\dx},{-0.8645*\dy}) + -- ({0.2002*\dx},{-0.8455*\dy}) + -- ({0.1855*\dx},{-0.8262*\dy}) + -- ({0.1712*\dx},{-0.8066*\dy}) + -- ({0.1573*\dx},{-0.7868*\dy}) + -- ({0.1440*\dx},{-0.7666*\dy}) + -- ({0.1311*\dx},{-0.7462*\dy}) + -- ({0.1187*\dx},{-0.7256*\dy}) + -- ({0.1068*\dx},{-0.7047*\dy}) + -- ({0.0953*\dx},{-0.6835*\dy}) + -- ({0.0844*\dx},{-0.6621*\dy}) + -- ({0.0740*\dx},{-0.6406*\dy}) + -- ({0.0641*\dx},{-0.6188*\dy}) + -- ({0.0547*\dx},{-0.5968*\dy}) + -- ({0.0458*\dx},{-0.5747*\dy}) + -- ({0.0375*\dx},{-0.5524*\dy}) + -- ({0.0296*\dx},{-0.5299*\dy}) + -- ({0.0223*\dx},{-0.5074*\dy}) + -- ({0.0156*\dx},{-0.4847*\dy}) + -- ({0.0093*\dx},{-0.4618*\dy}) + -- ({0.0037*\dx},{-0.4389*\dy}) + -- ({-0.0015*\dx},{-0.4159*\dy}) + -- ({-0.0061*\dx},{-0.3928*\dy}) + -- ({-0.0101*\dx},{-0.3697*\dy}) + -- ({-0.0136*\dx},{-0.3465*\dy}) + -- ({-0.0166*\dx},{-0.3233*\dy}) + -- ({-0.0190*\dx},{-0.3001*\dy}) + -- ({-0.0208*\dx},{-0.2768*\dy}) + -- ({-0.0221*\dx},{-0.2536*\dy}) + -- ({-0.0229*\dx},{-0.2304*\dy}) + -- ({-0.0231*\dx},{-0.2072*\dy}) + -- ({-0.0228*\dx},{-0.1841*\dy}) + -- ({-0.0219*\dx},{-0.1610*\dy}) + -- ({-0.0204*\dx},{-0.1380*\dy}) + -- ({-0.0185*\dx},{-0.1151*\dy}) + -- ({-0.0159*\dx},{-0.0923*\dy}) + -- ({-0.0129*\dx},{-0.0696*\dy}) + -- ({-0.0093*\dx},{-0.0470*\dy}) + -- ({-0.0052*\dx},{-0.0245*\dy}) + -- ({-0.0005*\dx},{-0.0023*\dy}) + -- ({0.0047*\dx},{0.0199*\dy}) + -- ({0.0104*\dx},{0.0418*\dy}) + -- ({0.0166*\dx},{0.0635*\dy}) + -- ({0.0233*\dx},{0.0851*\dy}) + -- ({0.0306*\dx},{0.1064*\dy}) + -- ({0.0383*\dx},{0.1275*\dy}) + -- ({0.0466*\dx},{0.1484*\dy}) + -- ({0.0553*\dx},{0.1690*\dy}) + -- ({0.0645*\dx},{0.1893*\dy}) + -- ({0.0742*\dx},{0.2094*\dy}) + -- ({0.0843*\dx},{0.2291*\dy}) + -- ({0.0950*\dx},{0.2486*\dy}) + -- ({0.1060*\dx},{0.2677*\dy}) + -- ({0.1176*\dx},{0.2866*\dy}) + -- ({0.1295*\dx},{0.3050*\dy}) + -- ({0.1419*\dx},{0.3232*\dy}) + -- ({0.1547*\dx},{0.3410*\dy}) + -- ({0.1679*\dx},{0.3584*\dy}) + -- ({0.1816*\dx},{0.3754*\dy}) + -- ({0.1956*\dx},{0.3921*\dy}) + -- ({0.2100*\dx},{0.4083*\dy}) + -- ({0.2248*\dx},{0.4242*\dy}) + -- ({0.2399*\dx},{0.4396*\dy}) + -- ({0.2554*\dx},{0.4546*\dy}) + -- ({0.2712*\dx},{0.4691*\dy}) + -- ({0.2874*\dx},{0.4832*\dy}) + -- ({0.3038*\dx},{0.4969*\dy}) + -- ({0.3206*\dx},{0.5101*\dy}) + -- ({0.3377*\dx},{0.5228*\dy}) + -- ({0.3550*\dx},{0.5351*\dy}) + -- ({0.3727*\dx},{0.5468*\dy}) + -- ({0.3906*\dx},{0.5581*\dy}) + -- ({0.4087*\dx},{0.5689*\dy}) + -- ({0.4270*\dx},{0.5792*\dy}) + -- ({0.4456*\dx},{0.5889*\dy}) + -- ({0.4644*\dx},{0.5982*\dy}) + -- ({0.4834*\dx},{0.6069*\dy}) + -- ({0.5025*\dx},{0.6151*\dy}) + -- ({0.5218*\dx},{0.6228*\dy}) + -- ({0.5413*\dx},{0.6299*\dy}) + -- ({0.5609*\dx},{0.6365*\dy}) + -- ({0.5806*\dx},{0.6426*\dy}) + -- ({0.6005*\dx},{0.6481*\dy}) + -- ({0.6204*\dx},{0.6531*\dy}) + -- ({0.6404*\dx},{0.6575*\dy}) + -- ({0.6605*\dx},{0.6614*\dy}) + -- ({0.6806*\dx},{0.6647*\dy}) + -- ({0.7007*\dx},{0.6674*\dy}) + -- ({0.7209*\dx},{0.6696*\dy}) + -- ({0.7411*\dx},{0.6713*\dy}) + -- ({0.7613*\dx},{0.6723*\dy}) + -- ({0.7814*\dx},{0.6729*\dy}) + -- ({0.8015*\dx},{0.6728*\dy}) + -- ({0.8216*\dx},{0.6722*\dy}) + -- ({0.8416*\dx},{0.6711*\dy}) + -- ({0.8615*\dx},{0.6694*\dy}) + -- ({0.8813*\dx},{0.6672*\dy}) + -- ({0.9010*\dx},{0.6644*\dy}) + -- ({0.9205*\dx},{0.6610*\dy}) + -- ({0.9400*\dx},{0.6571*\dy}) + -- ({0.9592*\dx},{0.6527*\dy}) + -- ({0.9783*\dx},{0.6478*\dy}) + -- ({0.9972*\dx},{0.6423*\dy}) + -- ({1.0159*\dx},{0.6363*\dy}) + -- ({1.0344*\dx},{0.6298*\dy}) + -- ({1.0527*\dx},{0.6227*\dy}) + -- ({1.0707*\dx},{0.6152*\dy}) + -- ({1.0885*\dx},{0.6071*\dy}) + -- ({1.1060*\dx},{0.5986*\dy}) + -- ({1.1232*\dx},{0.5896*\dy}) + -- ({1.1401*\dx},{0.5801*\dy}) + -- ({1.1567*\dx},{0.5701*\dy}) + -- ({1.1730*\dx},{0.5597*\dy}) + -- ({1.1889*\dx},{0.5488*\dy}) + -- ({1.2045*\dx},{0.5374*\dy}) + -- ({1.2197*\dx},{0.5257*\dy}) + -- ({1.2346*\dx},{0.5135*\dy}) + -- ({1.2491*\dx},{0.5008*\dy}) + -- ({1.2631*\dx},{0.4878*\dy}) + -- ({1.2768*\dx},{0.4744*\dy}) + -- ({1.2900*\dx},{0.4606*\dy}) + -- ({1.3029*\dx},{0.4464*\dy}) + -- ({1.3152*\dx},{0.4319*\dy}) + -- ({1.3271*\dx},{0.4170*\dy}) + -- ({1.3386*\dx},{0.4018*\dy}) + -- ({1.3496*\dx},{0.3862*\dy}) + -- ({1.3601*\dx},{0.3704*\dy}) + -- ({1.3701*\dx},{0.3542*\dy}) + -- ({1.3796*\dx},{0.3378*\dy}) + -- ({1.3886*\dx},{0.3211*\dy}) + -- ({1.3971*\dx},{0.3041*\dy}) + -- ({1.4051*\dx},{0.2869*\dy}) + -- ({1.4125*\dx},{0.2694*\dy}) + -- ({1.4195*\dx},{0.2518*\dy}) + -- ({1.4258*\dx},{0.2339*\dy}) + -- ({1.4316*\dx},{0.2159*\dy}) + -- ({1.4369*\dx},{0.1977*\dy}) + -- ({1.4416*\dx},{0.1793*\dy}) + -- ({1.4457*\dx},{0.1608*\dy}) + -- ({1.4493*\dx},{0.1422*\dy}) + -- ({1.4523*\dx},{0.1235*\dy}) + -- ({1.4547*\dx},{0.1047*\dy}) + -- ({1.4565*\dx},{0.0858*\dy}) + -- ({1.4577*\dx},{0.0668*\dy}) + -- ({1.4584*\dx},{0.0478*\dy}) + -- ({1.4584*\dx},{0.0288*\dy}) + -- ({1.4579*\dx},{0.0098*\dy}) + -- ({1.4568*\dx},{-0.0092*\dy}) + -- ({1.4551*\dx},{-0.0282*\dy}) + -- ({1.4528*\dx},{-0.0472*\dy}) + -- ({1.4499*\dx},{-0.0661*\dy}) + -- ({1.4464*\dx},{-0.0849*\dy}) + -- ({1.4424*\dx},{-0.1036*\dy}) + -- ({1.4377*\dx},{-0.1222*\dy}) + -- ({1.4325*\dx},{-0.1407*\dy}) + -- ({1.4267*\dx},{-0.1591*\dy}) + -- ({1.4202*\dx},{-0.1773*\dy}) + -- ({1.4133*\dx},{-0.1953*\dy}) + -- ({1.4057*\dx},{-0.2131*\dy}) + -- ({1.3976*\dx},{-0.2307*\dy}) + -- ({1.3889*\dx},{-0.2481*\dy}) + -- ({1.3797*\dx},{-0.2652*\dy}) + -- ({1.3699*\dx},{-0.2821*\dy}) + -- ({1.3595*\dx},{-0.2987*\dy}) + -- ({1.3487*\dx},{-0.3151*\dy}) + -- ({1.3373*\dx},{-0.3311*\dy}) + -- ({1.3253*\dx},{-0.3468*\dy}) + -- ({1.3129*\dx},{-0.3621*\dy}) + -- ({1.2999*\dx},{-0.3771*\dy}) + -- ({1.2865*\dx},{-0.3917*\dy}) + -- ({1.2725*\dx},{-0.4060*\dy}) + -- ({1.2581*\dx},{-0.4198*\dy}) + -- ({1.2432*\dx},{-0.4333*\dy}) + -- ({1.2279*\dx},{-0.4463*\dy}) + -- ({1.2121*\dx},{-0.4589*\dy}) + -- ({1.1959*\dx},{-0.4710*\dy}) + -- ({1.1792*\dx},{-0.4826*\dy}) + -- ({1.1622*\dx},{-0.4938*\dy}) + -- ({1.1447*\dx},{-0.5045*\dy}) + -- ({1.1269*\dx},{-0.5147*\dy}) + -- ({1.1087*\dx},{-0.5243*\dy}) + -- ({1.0901*\dx},{-0.5335*\dy}) + -- ({1.0712*\dx},{-0.5420*\dy}) + -- ({1.0520*\dx},{-0.5501*\dy}) + -- ({1.0324*\dx},{-0.5575*\dy}) + -- ({1.0126*\dx},{-0.5644*\dy}) + -- ({0.9924*\dx},{-0.5708*\dy}) + -- ({0.9721*\dx},{-0.5765*\dy}) + -- ({0.9514*\dx},{-0.5816*\dy}) + -- ({0.9305*\dx},{-0.5861*\dy}) + -- ({0.9094*\dx},{-0.5900*\dy}) + -- ({0.8881*\dx},{-0.5933*\dy}) + -- ({0.8666*\dx},{-0.5959*\dy}) + -- ({0.8450*\dx},{-0.5979*\dy}) + -- ({0.8232*\dx},{-0.5993*\dy}) + -- ({0.8013*\dx},{-0.6000*\dy}) + -- ({0.7792*\dx},{-0.6000*\dy}) + -- ({0.7571*\dx},{-0.5994*\dy}) + -- ({0.7349*\dx},{-0.5981*\dy}) + -- ({0.7126*\dx},{-0.5961*\dy}) + -- ({0.6903*\dx},{-0.5935*\dy}) + -- ({0.6680*\dx},{-0.5902*\dy}) + -- ({0.6457*\dx},{-0.5862*\dy}) + -- ({0.6234*\dx},{-0.5815*\dy}) + -- ({0.6012*\dx},{-0.5762*\dy}) + -- ({0.5790*\dx},{-0.5701*\dy}) + -- ({0.5568*\dx},{-0.5634*\dy}) + -- ({0.5348*\dx},{-0.5560*\dy}) + -- ({0.5129*\dx},{-0.5479*\dy}) + -- ({0.4911*\dx},{-0.5391*\dy}) + -- ({0.4695*\dx},{-0.5297*\dy}) + -- ({0.4481*\dx},{-0.5196*\dy}) + -- ({0.4269*\dx},{-0.5087*\dy}) + -- ({0.4058*\dx},{-0.4973*\dy}) + -- ({0.3850*\dx},{-0.4851*\dy}) + -- ({0.3645*\dx},{-0.4723*\dy}) + -- ({0.3442*\dx},{-0.4589*\dy}) + -- ({0.3243*\dx},{-0.4448*\dy}) + -- ({0.3046*\dx},{-0.4300*\dy}) + -- ({0.2853*\dx},{-0.4146*\dy}) + -- ({0.2663*\dx},{-0.3986*\dy}) + -- ({0.2477*\dx},{-0.3820*\dy}) + -- ({0.2295*\dx},{-0.3647*\dy}) + -- ({0.2117*\dx},{-0.3468*\dy}) + -- ({0.1943*\dx},{-0.3284*\dy}) + -- ({0.1774*\dx},{-0.3093*\dy}) + -- ({0.1609*\dx},{-0.2897*\dy}) + -- ({0.1449*\dx},{-0.2695*\dy}) + -- ({0.1294*\dx},{-0.2488*\dy}) + -- ({0.1144*\dx},{-0.2275*\dy}) + -- ({0.0999*\dx},{-0.2057*\dy}) + -- ({0.0860*\dx},{-0.1834*\dy}) + -- ({0.0726*\dx},{-0.1606*\dy}) + -- ({0.0598*\dx},{-0.1373*\dy}) + -- ({0.0476*\dx},{-0.1135*\dy}) + -- ({0.0360*\dx},{-0.0893*\dy}) + -- ({0.0250*\dx},{-0.0646*\dy}) + -- ({0.0147*\dx},{-0.0395*\dy}) + -- ({0.0050*\dx},{-0.0140*\dy}) + -- ({-0.0040*\dx},{0.0119*\dy}) + -- ({-0.0124*\dx},{0.0382*\dy}) + -- ({-0.0201*\dx},{0.0648*\dy}) + -- ({-0.0270*\dx},{0.0918*\dy}) + -- ({-0.0333*\dx},{0.1191*\dy}) + -- ({-0.0388*\dx},{0.1466*\dy}) + -- ({-0.0436*\dx},{0.1745*\dy}) + -- ({-0.0477*\dx},{0.2027*\dy}) + -- ({-0.0510*\dx},{0.2311*\dy}) + -- ({-0.0535*\dx},{0.2597*\dy}) + -- ({-0.0553*\dx},{0.2885*\dy}) + -- ({-0.0563*\dx},{0.3175*\dy}) + -- ({-0.0565*\dx},{0.3466*\dy}) + -- ({-0.0559*\dx},{0.3759*\dy}) + -- ({-0.0545*\dx},{0.4054*\dy}) + -- ({-0.0523*\dx},{0.4349*\dy}) + -- ({-0.0494*\dx},{0.4645*\dy}) + -- ({-0.0455*\dx},{0.4941*\dy}) + -- ({-0.0409*\dx},{0.5238*\dy}) + -- ({-0.0355*\dx},{0.5535*\dy}) + -- ({-0.0292*\dx},{0.5832*\dy}) + -- ({-0.0221*\dx},{0.6128*\dy}) + -- ({-0.0142*\dx},{0.6424*\dy}) + -- ({-0.0054*\dx},{0.6719*\dy}) + -- ({0.0042*\dx},{0.7013*\dy}) + -- ({0.0146*\dx},{0.7305*\dy}) + -- ({0.0258*\dx},{0.7597*\dy}) + -- ({0.0379*\dx},{0.7886*\dy}) + -- ({0.0508*\dx},{0.8174*\dy}) + -- ({0.0645*\dx},{0.8459*\dy}) + -- ({0.0790*\dx},{0.8742*\dy}) + -- ({0.0943*\dx},{0.9022*\dy}) + -- ({0.1105*\dx},{0.9299*\dy}) + -- ({0.1274*\dx},{0.9573*\dy}) + -- ({0.1452*\dx},{0.9844*\dy}) + -- ({0.1637*\dx},{1.0111*\dy}) + -- ({0.1830*\dx},{1.0375*\dy}) + -- ({0.2031*\dx},{1.0634*\dy}) + -- ({0.2239*\dx},{1.0889*\dy}) + -- ({0.2455*\dx},{1.1140*\dy}) + -- ({0.2679*\dx},{1.1386*\dy}) + -- ({0.2910*\dx},{1.1627*\dy}) + -- ({0.3148*\dx},{1.1863*\dy}) + -- ({0.3393*\dx},{1.2094*\dy}) + -- ({0.3645*\dx},{1.2319*\dy}) + -- ({0.3904*\dx},{1.2539*\dy}) + -- ({0.4169*\dx},{1.2752*\dy}) + -- ({0.4442*\dx},{1.2960*\dy}) + -- ({0.4720*\dx},{1.3161*\dy}) + -- ({0.5005*\dx},{1.3355*\dy}) + -- ({0.5296*\dx},{1.3543*\dy}) + -- ({0.5593*\dx},{1.3724*\dy}) + -- ({0.5896*\dx},{1.3898*\dy}) + -- ({0.6204*\dx},{1.4065*\dy}) + -- ({0.6518*\dx},{1.4224*\dy}) + -- ({0.6837*\dx},{1.4376*\dy}) + -- ({0.7161*\dx},{1.4520*\dy}) + -- ({0.7489*\dx},{1.4656*\dy}) + -- ({0.7823*\dx},{1.4784*\dy}) + -- ({0.8160*\dx},{1.4903*\dy}) + -- ({0.8503*\dx},{1.5015*\dy}) + -- ({0.8849*\dx},{1.5118*\dy}) + -- ({0.9198*\dx},{1.5213*\dy}) + -- ({0.9552*\dx},{1.5298*\dy}) + -- ({0.9908*\dx},{1.5375*\dy}) + -- ({1.0268*\dx},{1.5443*\dy}) + -- ({1.0631*\dx},{1.5502*\dy}) + -- ({1.0996*\dx},{1.5552*\dy}) + -- ({1.1364*\dx},{1.5593*\dy}) + -- ({1.1733*\dx},{1.5624*\dy}) + -- ({1.2105*\dx},{1.5646*\dy}) + -- ({1.2478*\dx},{1.5658*\dy}) + -- ({1.2853*\dx},{1.5661*\dy}) + -- ({1.3229*\dx},{1.5655*\dy}) + -- ({1.3606*\dx},{1.5638*\dy}) + -- ({1.3983*\dx},{1.5613*\dy}) + -- ({1.4361*\dx},{1.5577*\dy}) + -- ({1.4738*\dx},{1.5531*\dy}) + -- ({1.5116*\dx},{1.5476*\dy}) + -- ({1.5493*\dx},{1.5411*\dy}) + -- ({1.5870*\dx},{1.5337*\dy}) + -- ({1.6245*\dx},{1.5252*\dy}) + -- ({1.6620*\dx},{1.5158*\dy}) + -- ({1.6993*\dx},{1.5054*\dy}) + -- ({1.7364*\dx},{1.4940*\dy}) + -- ({1.7733*\dx},{1.4816*\dy}) + -- ({1.8100*\dx},{1.4683*\dy}) + -- ({1.8464*\dx},{1.4540*\dy}) + -- ({1.8826*\dx},{1.4388*\dy}) + -- ({1.9184*\dx},{1.4226*\dy}) + -- ({1.9539*\dx},{1.4055*\dy}) + -- ({1.9891*\dx},{1.3874*\dy}) + -- ({2.0238*\dx},{1.3684*\dy}) + -- ({2.0582*\dx},{1.3484*\dy}) + -- ({2.0921*\dx},{1.3276*\dy}) + -- ({2.1255*\dx},{1.3059*\dy}) + -- ({2.1585*\dx},{1.2832*\dy}) + -- ({2.1910*\dx},{1.2597*\dy}) + -- ({2.2229*\dx},{1.2353*\dy}) + -- ({2.2543*\dx},{1.2101*\dy}) + -- ({2.2850*\dx},{1.1840*\dy}) + -- ({2.3152*\dx},{1.1571*\dy}) + -- ({2.3448*\dx},{1.1294*\dy}) + -- ({2.3736*\dx},{1.1009*\dy}) + -- ({2.4019*\dx},{1.0716*\dy}) + -- ({2.4294*\dx},{1.0416*\dy}) + -- ({2.4562*\dx},{1.0108*\dy}) + -- ({2.4822*\dx},{0.9793*\dy}) + -- ({2.5075*\dx},{0.9471*\dy}) + -- ({2.5321*\dx},{0.9142*\dy}) + -- ({2.5558*\dx},{0.8807*\dy}) + -- ({2.5787*\dx},{0.8465*\dy}) + -- ({2.6008*\dx},{0.8117*\dy}) + -- ({2.6220*\dx},{0.7762*\dy}) + -- ({2.6423*\dx},{0.7402*\dy}) + -- ({2.6618*\dx},{0.7037*\dy}) + -- ({2.6803*\dx},{0.6666*\dy}) + -- ({2.6980*\dx},{0.6290*\dy}) + -- ({2.7147*\dx},{0.5909*\dy}) + -- ({2.7305*\dx},{0.5524*\dy}) + -- ({2.7453*\dx},{0.5134*\dy}) + -- ({2.7591*\dx},{0.4740*\dy}) + -- ({2.7719*\dx},{0.4342*\dy}) + -- ({2.7838*\dx},{0.3941*\dy}) + -- ({2.7946*\dx},{0.3537*\dy}) + -- ({2.8045*\dx},{0.3129*\dy}) + -- ({2.8133*\dx},{0.2719*\dy}) + -- ({2.8210*\dx},{0.2306*\dy}) + -- ({2.8278*\dx},{0.1891*\dy}) + -- ({2.8335*\dx},{0.1474*\dy}) + -- ({2.8381*\dx},{0.1055*\dy}) + -- ({2.8417*\dx},{0.0636*\dy}) + -- ({2.8442*\dx},{0.0215*\dy}) + -- ({2.8457*\dx},{-0.0207*\dy}) + -- ({2.8461*\dx},{-0.0629*\dy}) + -- ({2.8454*\dx},{-0.1052*\dy}) + -- ({2.8436*\dx},{-0.1474*\dy}) + -- ({2.8408*\dx},{-0.1896*\dy}) + -- ({2.8369*\dx},{-0.2317*\dy}) + -- ({2.8320*\dx},{-0.2738*\dy}) + -- ({2.8260*\dx},{-0.3157*\dy}) + -- ({2.8189*\dx},{-0.3574*\dy}) + -- ({2.8108*\dx},{-0.3990*\dy}) + -- ({2.8016*\dx},{-0.4404*\dy}) + -- ({2.7914*\dx},{-0.4815*\dy}) + -- ({2.7801*\dx},{-0.5224*\dy}) + -- ({2.7678*\dx},{-0.5629*\dy}) + -- ({2.7545*\dx},{-0.6032*\dy}) + -- ({2.7401*\dx},{-0.6430*\dy}) + -- ({2.7248*\dx},{-0.6825*\dy}) + -- ({2.7084*\dx},{-0.7216*\dy}) + -- ({2.6911*\dx},{-0.7603*\dy}) + -- ({2.6728*\dx},{-0.7985*\dy}) + -- ({2.6535*\dx},{-0.8362*\dy}) + -- ({2.6333*\dx},{-0.8734*\dy}) + -- ({2.6122*\dx},{-0.9100*\dy}) + -- ({2.5901*\dx},{-0.9461*\dy}) + -- ({2.5671*\dx},{-0.9816*\dy}) + -- ({2.5433*\dx},{-1.0165*\dy}) + -- ({2.5186*\dx},{-1.0507*\dy}) + -- ({2.4930*\dx},{-1.0843*\dy}) + -- ({2.4667*\dx},{-1.1172*\dy}) + -- ({2.4395*\dx},{-1.1494*\dy}) + -- ({2.4115*\dx},{-1.1808*\dy}) + -- ({2.3827*\dx},{-1.2115*\dy}) + -- ({2.3532*\dx},{-1.2414*\dy}) + -- ({2.3230*\dx},{-1.2706*\dy}) + -- ({2.2921*\dx},{-1.2989*\dy}) + -- ({2.2605*\dx},{-1.3264*\dy}) + -- ({2.2282*\dx},{-1.3530*\dy}) + -- ({2.1953*\dx},{-1.3788*\dy}) + -- ({2.1618*\dx},{-1.4037*\dy}) + -- ({2.1277*\dx},{-1.4277*\dy}) + -- ({2.0930*\dx},{-1.4508*\dy}) + -- ({2.0578*\dx},{-1.4729*\dy}) + -- ({2.0221*\dx},{-1.4941*\dy}) + -- ({1.9859*\dx},{-1.5144*\dy}) + -- ({1.9493*\dx},{-1.5337*\dy}) + -- ({1.9123*\dx},{-1.5520*\dy}) + -- ({1.8748*\dx},{-1.5693*\dy}) + -- ({1.8370*\dx},{-1.5856*\dy}) + -- ({1.7988*\dx},{-1.6009*\dy}) + -- ({1.7604*\dx},{-1.6152*\dy}) + -- ({1.7216*\dx},{-1.6285*\dy}) + -- ({1.6826*\dx},{-1.6407*\dy}) + -- ({1.6434*\dx},{-1.6519*\dy}) + -- ({1.6040*\dx},{-1.6620*\dy}) + -- ({1.5644*\dx},{-1.6711*\dy}) + -- ({1.5247*\dx},{-1.6792*\dy}) + -- ({1.4848*\dx},{-1.6862*\dy}) + -- ({1.4449*\dx},{-1.6921*\dy}) + -- ({1.4050*\dx},{-1.6970*\dy}) + -- ({1.3650*\dx},{-1.7009*\dy}) + -- ({1.3250*\dx},{-1.7037*\dy}) + -- ({1.2851*\dx},{-1.7054*\dy}) + -- ({1.2453*\dx},{-1.7061*\dy}) + -- ({1.2056*\dx},{-1.7058*\dy}) + -- ({1.1660*\dx},{-1.7044*\dy}) + -- ({1.1265*\dx},{-1.7020*\dy}) + -- ({1.0873*\dx},{-1.6986*\dy}) + -- ({1.0482*\dx},{-1.6941*\dy}) + -- ({1.0095*\dx},{-1.6887*\dy}) + -- ({0.9709*\dx},{-1.6822*\dy}) + -- ({0.9327*\dx},{-1.6747*\dy}) + -- ({0.8949*\dx},{-1.6663*\dy}) + -- ({0.8574*\dx},{-1.6569*\dy}) + -- ({0.8202*\dx},{-1.6466*\dy}) + -- ({0.7835*\dx},{-1.6353*\dy}) + -- ({0.7473*\dx},{-1.6231*\dy}) + -- ({0.7115*\dx},{-1.6099*\dy}) + -- ({0.6761*\dx},{-1.5959*\dy}) + -- ({0.6413*\dx},{-1.5810*\dy}) + -- ({0.6071*\dx},{-1.5652*\dy}) + -- ({0.5734*\dx},{-1.5486*\dy}) + -- ({0.5403*\dx},{-1.5312*\dy}) + -- ({0.5078*\dx},{-1.5129*\dy}) + -- ({0.4759*\dx},{-1.4939*\dy}) + -- ({0.4447*\dx},{-1.4741*\dy}) + -- ({0.4141*\dx},{-1.4535*\dy}) + -- ({0.3843*\dx},{-1.4322*\dy}) + -- ({0.3552*\dx},{-1.4103*\dy}) + -- ({0.3268*\dx},{-1.3876*\dy}) + -- ({0.2991*\dx},{-1.3643*\dy}) + -- ({0.2722*\dx},{-1.3403*\dy}) + -- ({0.2461*\dx},{-1.3158*\dy}) + -- ({0.2208*\dx},{-1.2907*\dy}) + -- ({0.1963*\dx},{-1.2650*\dy}) + -- ({0.1726*\dx},{-1.2387*\dy}) + -- ({0.1498*\dx},{-1.2120*\dy}) + -- ({0.1279*\dx},{-1.1848*\dy}) + -- ({0.1068*\dx},{-1.1572*\dy}) + -- ({0.0865*\dx},{-1.1291*\dy}) + -- ({0.0672*\dx},{-1.1006*\dy}) + -- ({0.0487*\dx},{-1.0718*\dy}) + -- ({0.0312*\dx},{-1.0426*\dy}) + -- ({0.0146*\dx},{-1.0131*\dy}) + -- ({-0.0011*\dx},{-0.9833*\dy}) + -- ({-0.0159*\dx},{-0.9533*\dy}) + -- ({-0.0298*\dx},{-0.9230*\dy}) + -- ({-0.0427*\dx},{-0.8926*\dy}) + -- ({-0.0547*\dx},{-0.8620*\dy}) + -- ({-0.0658*\dx},{-0.8312*\dy}) + -- ({-0.0759*\dx},{-0.8003*\dy}) + -- ({-0.0851*\dx},{-0.7694*\dy}) + -- ({-0.0933*\dx},{-0.7384*\dy}) + -- ({-0.1007*\dx},{-0.7074*\dy}) + -- ({-0.1070*\dx},{-0.6764*\dy}) + -- ({-0.1125*\dx},{-0.6454*\dy}) + -- ({-0.1170*\dx},{-0.6145*\dy}) + -- ({-0.1206*\dx},{-0.5837*\dy}) + -- ({-0.1233*\dx},{-0.5530*\dy}) + -- ({-0.1251*\dx},{-0.5225*\dy}) + -- ({-0.1260*\dx},{-0.4921*\dy}) + -- ({-0.1261*\dx},{-0.4619*\dy}) + -- ({-0.1252*\dx},{-0.4320*\dy}) + -- ({-0.1235*\dx},{-0.4024*\dy}) + -- ({-0.1209*\dx},{-0.3730*\dy}) + -- ({-0.1175*\dx},{-0.3439*\dy}) + -- ({-0.1132*\dx},{-0.3152*\dy}) + -- ({-0.1081*\dx},{-0.2868*\dy}) + -- ({-0.1022*\dx},{-0.2589*\dy}) + -- ({-0.0956*\dx},{-0.2313*\dy}) + -- ({-0.0882*\dx},{-0.2042*\dy}) + -- ({-0.0800*\dx},{-0.1775*\dy}) + -- ({-0.0711*\dx},{-0.1513*\dy}) + -- ({-0.0614*\dx},{-0.1256*\dy}) + -- ({-0.0511*\dx},{-0.1005*\dy}) + -- ({-0.0401*\dx},{-0.0759*\dy}) + -- ({-0.0284*\dx},{-0.0518*\dy}) + -- ({-0.0161*\dx},{-0.0283*\dy}) + -- ({-0.0032*\dx},{-0.0055*\dy}) + -- ({0.0103*\dx},{0.0168*\dy}) + -- ({0.0243*\dx},{0.0384*\dy}) + -- ({0.0389*\dx},{0.0593*\dy}) + -- ({0.0541*\dx},{0.0796*\dy}) + -- ({0.0697*\dx},{0.0992*\dy}) + -- ({0.0858*\dx},{0.1181*\dy}) + -- ({0.1023*\dx},{0.1363*\dy}) + -- ({0.1193*\dx},{0.1537*\dy}) + -- ({0.1367*\dx},{0.1705*\dy}) + -- ({0.1544*\dx},{0.1864*\dy}) + -- ({0.1725*\dx},{0.2017*\dy}) + -- ({0.1908*\dx},{0.2161*\dy}) + -- ({0.2095*\dx},{0.2298*\dy}) + -- ({0.2284*\dx},{0.2427*\dy}) + -- ({0.2476*\dx},{0.2549*\dy}) + -- ({0.2669*\dx},{0.2662*\dy}) + -- ({0.2865*\dx},{0.2768*\dy}) + -- ({0.3062*\dx},{0.2865*\dy}) + -- ({0.3260*\dx},{0.2955*\dy}) + -- ({0.3459*\dx},{0.3036*\dy}) + -- ({0.3658*\dx},{0.3110*\dy}) + -- ({0.3858*\dx},{0.3175*\dy}) + -- ({0.4058*\dx},{0.3233*\dy}) + -- ({0.4258*\dx},{0.3283*\dy}) + -- ({0.4457*\dx},{0.3324*\dy}) + -- ({0.4655*\dx},{0.3358*\dy}) + -- ({0.4853*\dx},{0.3384*\dy}) + -- ({0.5049*\dx},{0.3403*\dy}) + -- ({0.5243*\dx},{0.3413*\dy}) + -- ({0.5436*\dx},{0.3416*\dy}) + -- ({0.5626*\dx},{0.3412*\dy}) + -- ({0.5814*\dx},{0.3400*\dy}) + -- ({0.5999*\dx},{0.3381*\dy}) + -- ({0.6182*\dx},{0.3355*\dy}) + -- ({0.6361*\dx},{0.3321*\dy}) + -- ({0.6537*\dx},{0.3281*\dy}) + -- ({0.6709*\dx},{0.3234*\dy}) + -- ({0.6877*\dx},{0.3181*\dy}) + -- ({0.7041*\dx},{0.3120*\dy}) + -- ({0.7201*\dx},{0.3054*\dy}) + -- ({0.7356*\dx},{0.2982*\dy}) + -- ({0.7506*\dx},{0.2903*\dy}) + -- ({0.7651*\dx},{0.2819*\dy}) + -- ({0.7791*\dx},{0.2730*\dy}) + -- ({0.7926*\dx},{0.2635*\dy}) + -- ({0.8055*\dx},{0.2535*\dy}) + -- ({0.8178*\dx},{0.2430*\dy}) + -- ({0.8296*\dx},{0.2320*\dy}) + -- ({0.8407*\dx},{0.2206*\dy}) + -- ({0.8512*\dx},{0.2088*\dy}) + -- ({0.8610*\dx},{0.1965*\dy}) + -- ({0.8702*\dx},{0.1839*\dy}) + -- ({0.8788*\dx},{0.1710*\dy}) + -- ({0.8866*\dx},{0.1577*\dy}) + -- ({0.8937*\dx},{0.1442*\dy}) + -- ({0.9002*\dx},{0.1304*\dy}) + -- ({0.9059*\dx},{0.1163*\dy}) + -- ({0.9109*\dx},{0.1020*\dy}) + -- ({0.9152*\dx},{0.0876*\dy}) + -- ({0.9187*\dx},{0.0730*\dy}) + -- ({0.9215*\dx},{0.0582*\dy}) + -- ({0.9236*\dx},{0.0434*\dy}) + -- ({0.9249*\dx},{0.0284*\dy}) + -- ({0.9254*\dx},{0.0135*\dy}) + -- ({0.9252*\dx},{-0.0015*\dy}) + -- ({0.9242*\dx},{-0.0165*\dy}) + -- ({0.9225*\dx},{-0.0314*\dy}) + -- ({0.9200*\dx},{-0.0463*\dy}) + -- ({0.9168*\dx},{-0.0610*\dy}) + -- ({0.9128*\dx},{-0.0756*\dy}) + -- ({0.9081*\dx},{-0.0901*\dy}) + -- ({0.9026*\dx},{-0.1044*\dy}) + -- ({0.8964*\dx},{-0.1184*\dy}) + -- ({0.8895*\dx},{-0.1322*\dy}) + -- ({0.8818*\dx},{-0.1458*\dy}) + -- ({0.8734*\dx},{-0.1590*\dy}) + -- ({0.8644*\dx},{-0.1720*\dy}) + -- ({0.8546*\dx},{-0.1845*\dy}) + -- ({0.8442*\dx},{-0.1967*\dy}) + -- ({0.8331*\dx},{-0.2085*\dy}) + -- ({0.8214*\dx},{-0.2198*\dy}) + -- ({0.8090*\dx},{-0.2307*\dy}) + -- ({0.7960*\dx},{-0.2411*\dy}) + -- ({0.7824*\dx},{-0.2510*\dy}) + -- ({0.7682*\dx},{-0.2603*\dy}) + -- ({0.7535*\dx},{-0.2691*\dy}) + -- ({0.7382*\dx},{-0.2773*\dy}) + -- ({0.7224*\dx},{-0.2849*\dy}) + -- ({0.7061*\dx},{-0.2919*\dy}) + -- ({0.6893*\dx},{-0.2982*\dy}) + -- ({0.6721*\dx},{-0.3039*\dy}) + -- ({0.6544*\dx},{-0.3089*\dy}) + -- ({0.6363*\dx},{-0.3132*\dy}) + -- ({0.6178*\dx},{-0.3168*\dy}) + -- ({0.5989*\dx},{-0.3196*\dy}) + -- ({0.5798*\dx},{-0.3217*\dy}) + -- ({0.5603*\dx},{-0.3230*\dy}) + -- ({0.5405*\dx},{-0.3235*\dy}) + -- ({0.5205*\dx},{-0.3232*\dy}) + -- ({0.5003*\dx},{-0.3222*\dy}) + -- ({0.4798*\dx},{-0.3203*\dy}) + -- ({0.4592*\dx},{-0.3175*\dy}) + -- ({0.4385*\dx},{-0.3140*\dy}) + -- ({0.4176*\dx},{-0.3095*\dy}) + -- ({0.3967*\dx},{-0.3043*\dy}) + -- ({0.3758*\dx},{-0.2981*\dy}) + -- ({0.3548*\dx},{-0.2911*\dy}) + -- ({0.3338*\dx},{-0.2832*\dy}) + -- ({0.3129*\dx},{-0.2745*\dy}) + -- ({0.2921*\dx},{-0.2649*\dy}) + -- ({0.2714*\dx},{-0.2544*\dy}) + -- ({0.2508*\dx},{-0.2430*\dy}) + -- ({0.2305*\dx},{-0.2307*\dy}) + -- ({0.2103*\dx},{-0.2176*\dy}) + -- ({0.1904*\dx},{-0.2036*\dy}) + -- ({0.1707*\dx},{-0.1887*\dy}) + -- ({0.1514*\dx},{-0.1730*\dy}) + -- ({0.1324*\dx},{-0.1564*\dy}) + -- ({0.1137*\dx},{-0.1390*\dy}) + -- ({0.0955*\dx},{-0.1207*\dy}) + -- ({0.0777*\dx},{-0.1016*\dy}) + -- ({0.0604*\dx},{-0.0817*\dy}) + -- ({0.0435*\dx},{-0.0610*\dy}) + -- ({0.0272*\dx},{-0.0395*\dy}) + -- ({0.0115*\dx},{-0.0173*\dy}) + -- ({-0.0037*\dx},{0.0058*\dy}) + -- ({-0.0182*\dx},{0.0295*\dy}) + -- ({-0.0321*\dx},{0.0540*\dy}) + -- ({-0.0454*\dx},{0.0792*\dy}) + -- ({-0.0579*\dx},{0.1051*\dy}) + -- ({-0.0697*\dx},{0.1316*\dy}) + -- ({-0.0807*\dx},{0.1588*\dy}) + -- ({-0.0910*\dx},{0.1866*\dy}) + -- ({-0.1005*\dx},{0.2150*\dy}) + -- ({-0.1091*\dx},{0.2439*\dy}) + -- ({-0.1169*\dx},{0.2734*\dy}) + -- ({-0.1238*\dx},{0.3035*\dy}) + -- ({-0.1298*\dx},{0.3340*\dy}) + -- ({-0.1349*\dx},{0.3649*\dy}) + -- ({-0.1391*\dx},{0.3964*\dy}) + -- ({-0.1423*\dx},{0.4282*\dy}) + -- ({-0.1445*\dx},{0.4604*\dy}) + -- ({-0.1457*\dx},{0.4929*\dy}) + -- ({-0.1459*\dx},{0.5257*\dy}) + -- ({-0.1451*\dx},{0.5589*\dy}) + -- ({-0.1433*\dx},{0.5922*\dy}) + -- ({-0.1404*\dx},{0.6258*\dy}) + -- ({-0.1365*\dx},{0.6595*\dy}) + -- ({-0.1314*\dx},{0.6934*\dy}) + -- ({-0.1253*\dx},{0.7274*\dy}) + -- ({-0.1181*\dx},{0.7615*\dy}) + -- ({-0.1098*\dx},{0.7956*\dy}) + -- ({-0.1004*\dx},{0.8298*\dy}) + -- ({-0.0899*\dx},{0.8638*\dy}) + -- ({-0.0783*\dx},{0.8978*\dy}) + -- ({-0.0655*\dx},{0.9317*\dy}) + -- ({-0.0517*\dx},{0.9655*\dy}) + -- ({-0.0367*\dx},{0.9990*\dy}) + -- ({-0.0206*\dx},{1.0324*\dy}) + -- ({-0.0034*\dx},{1.0654*\dy}) + -- ({0.0149*\dx},{1.0982*\dy}) + -- ({0.0344*\dx},{1.1307*\dy}) + -- ({0.0549*\dx},{1.1627*\dy}) + -- ({0.0765*\dx},{1.1944*\dy}) + -- ({0.0992*\dx},{1.2256*\dy}) + -- ({0.1230*\dx},{1.2563*\dy}) + -- ({0.1478*\dx},{1.2865*\dy}) + -- ({0.1737*\dx},{1.3162*\dy}) + -- ({0.2006*\dx},{1.3452*\dy}) + -- ({0.2285*\dx},{1.3737*\dy}) + -- ({0.2574*\dx},{1.4014*\dy}) + -- ({0.2874*\dx},{1.4285*\dy}) + -- ({0.3182*\dx},{1.4548*\dy}) + -- ({0.3501*\dx},{1.4804*\dy}) + -- ({0.3828*\dx},{1.5051*\dy}) + -- ({0.4165*\dx},{1.5291*\dy}) + -- ({0.4510*\dx},{1.5521*\dy}) + -- ({0.4864*\dx},{1.5743*\dy}) + -- ({0.5226*\dx},{1.5955*\dy}) + -- ({0.5597*\dx},{1.6158*\dy}) + -- ({0.5975*\dx},{1.6350*\dy}) + -- ({0.6360*\dx},{1.6533*\dy}) + -- ({0.6753*\dx},{1.6705*\dy}) + -- ({0.7152*\dx},{1.6867*\dy}) + -- ({0.7558*\dx},{1.7017*\dy}) + -- ({0.7970*\dx},{1.7157*\dy}) + -- ({0.8388*\dx},{1.7285*\dy}) + -- ({0.8812*\dx},{1.7401*\dy}) + -- ({0.9241*\dx},{1.7505*\dy}) + -- ({0.9674*\dx},{1.7598*\dy}) + -- ({1.0112*\dx},{1.7678*\dy}) + -- ({1.0554*\dx},{1.7746*\dy}) + -- ({1.1000*\dx},{1.7801*\dy}) + -- ({1.1449*\dx},{1.7843*\dy}) + -- ({1.1901*\dx},{1.7872*\dy}) + -- ({1.2355*\dx},{1.7889*\dy}) + -- ({1.2812*\dx},{1.7892*\dy}) + -- ({1.3270*\dx},{1.7882*\dy}) + -- ({1.3730*\dx},{1.7859*\dy}) + -- ({1.4190*\dx},{1.7822*\dy}) + -- ({1.4651*\dx},{1.7772*\dy}) + -- ({1.5111*\dx},{1.7708*\dy}) + -- ({1.5572*\dx},{1.7631*\dy}) + -- ({1.6031*\dx},{1.7540*\dy}) + -- ({1.6490*\dx},{1.7435*\dy}) + -- ({1.6946*\dx},{1.7317*\dy}) + -- ({1.7400*\dx},{1.7185*\dy}) + -- ({1.7852*\dx},{1.7040*\dy}) + -- ({1.8301*\dx},{1.6882*\dy}) + -- ({1.8746*\dx},{1.6709*\dy}) + -- ({1.9188*\dx},{1.6524*\dy}) + -- ({1.9625*\dx},{1.6325*\dy}) + -- ({2.0058*\dx},{1.6114*\dy}) + -- ({2.0485*\dx},{1.5889*\dy}) + -- ({2.0907*\dx},{1.5651*\dy}) + -- ({2.1322*\dx},{1.5401*\dy}) + -- ({2.1732*\dx},{1.5138*\dy}) + -- ({2.2134*\dx},{1.4862*\dy}) + -- ({2.2530*\dx},{1.4574*\dy}) + -- ({2.2918*\dx},{1.4275*\dy}) + -- ({2.3297*\dx},{1.3963*\dy}) + -- ({2.3669*\dx},{1.3640*\dy}) + -- ({2.4031*\dx},{1.3306*\dy}) + -- ({2.4385*\dx},{1.2961*\dy}) + -- ({2.4729*\dx},{1.2605*\dy}) + -- ({2.5063*\dx},{1.2238*\dy}) + -- ({2.5387*\dx},{1.1861*\dy}) + -- ({2.5701*\dx},{1.1474*\dy}) + -- ({2.6003*\dx},{1.1078*\dy}) + -- ({2.6295*\dx},{1.0672*\dy}) + -- ({2.6575*\dx},{1.0258*\dy}) + -- ({2.6843*\dx},{0.9835*\dy}) + -- ({2.7099*\dx},{0.9403*\dy}) + -- ({2.7343*\dx},{0.8964*\dy}) + -- ({2.7574*\dx},{0.8517*\dy}) + -- ({2.7793*\dx},{0.8063*\dy}) + -- ({2.7998*\dx},{0.7603*\dy}) + -- ({2.8190*\dx},{0.7136*\dy}) + -- ({2.8369*\dx},{0.6663*\dy}) + -- ({2.8534*\dx},{0.6185*\dy}) + -- ({2.8684*\dx},{0.5702*\dy}) + -- ({2.8821*\dx},{0.5214*\dy}) + -- ({2.8944*\dx},{0.4722*\dy}) + -- ({2.9052*\dx},{0.4227*\dy}) + -- ({2.9146*\dx},{0.3728*\dy}) + -- ({2.9225*\dx},{0.3226*\dy}) + -- ({2.9289*\dx},{0.2722*\dy}) + -- ({2.9339*\dx},{0.2216*\dy}) + -- ({2.9374*\dx},{0.1709*\dy}) + -- ({2.9394*\dx},{0.1200*\dy}) + -- ({2.9399*\dx},{0.0692*\dy}) + -- ({2.9389*\dx},{0.0183*\dy}) + -- ({2.9363*\dx},{-0.0326*\dy}) + -- ({2.9323*\dx},{-0.0833*\dy}) + -- ({2.9268*\dx},{-0.1339*\dy}) + -- ({2.9198*\dx},{-0.1843*\dy}) + -- ({2.9114*\dx},{-0.2345*\dy}) + -- ({2.9014*\dx},{-0.2844*\dy}) + -- ({2.8900*\dx},{-0.3340*\dy}) + -- ({2.8771*\dx},{-0.3832*\dy}) + -- ({2.8627*\dx},{-0.4319*\dy}) + -- ({2.8470*\dx},{-0.4802*\dy}) + -- ({2.8298*\dx},{-0.5280*\dy}) + -- ({2.8112*\dx},{-0.5753*\dy}) + -- ({2.7912*\dx},{-0.6219*\dy}) + -- ({2.7698*\dx},{-0.6679*\dy}) + -- ({2.7471*\dx},{-0.7131*\dy}) + -- ({2.7231*\dx},{-0.7577*\dy}) + -- ({2.6978*\dx},{-0.8015*\dy}) + -- ({2.6712*\dx},{-0.8444*\dy}) + -- ({2.6433*\dx},{-0.8865*\dy}) + -- ({2.6143*\dx},{-0.9277*\dy}) + -- ({2.5840*\dx},{-0.9680*\dy}) + -- ({2.5526*\dx},{-1.0073*\dy}) + -- ({2.5200*\dx},{-1.0455*\dy}) + -- ({2.4863*\dx},{-1.0828*\dy}) + -- ({2.4516*\dx},{-1.1189*\dy}) + -- ({2.4159*\dx},{-1.1539*\dy}) + -- ({2.3791*\dx},{-1.1878*\dy}) + -- ({2.3414*\dx},{-1.2205*\dy}) + -- ({2.3028*\dx},{-1.2520*\dy}) + -- ({2.2633*\dx},{-1.2823*\dy}) + -- ({2.2230*\dx},{-1.3113*\dy}) + -- ({2.1819*\dx},{-1.3390*\dy}) + -- ({2.1400*\dx},{-1.3654*\dy}) + -- ({2.0974*\dx},{-1.3904*\dy}) + -- ({2.0542*\dx},{-1.4141*\dy}) + -- ({2.0103*\dx},{-1.4364*\dy}) + -- ({1.9659*\dx},{-1.4573*\dy}) + -- ({1.9209*\dx},{-1.4768*\dy}) + -- ({1.8755*\dx},{-1.4948*\dy}) + -- ({1.8296*\dx},{-1.5114*\dy}) + -- ({1.7833*\dx},{-1.5266*\dy}) + -- ({1.7367*\dx},{-1.5402*\dy}) + -- ({1.6897*\dx},{-1.5524*\dy}) + -- ({1.6426*\dx},{-1.5631*\dy}) + -- ({1.5952*\dx},{-1.5723*\dy}) + -- ({1.5477*\dx},{-1.5800*\dy}) + -- ({1.5001*\dx},{-1.5862*\dy}) + -- ({1.4524*\dx},{-1.5909*\dy}) + -- ({1.4048*\dx},{-1.5941*\dy}) + -- ({1.3572*\dx},{-1.5958*\dy}) + -- ({1.3097*\dx},{-1.5960*\dy}) + -- ({1.2623*\dx},{-1.5947*\dy}) + -- ({1.2152*\dx},{-1.5919*\dy}) + -- ({1.1683*\dx},{-1.5876*\dy}) + -- ({1.1217*\dx},{-1.5818*\dy}) + -- ({1.0754*\dx},{-1.5747*\dy}) + -- ({1.0295*\dx},{-1.5660*\dy}) + -- ({0.9841*\dx},{-1.5559*\dy}) + -- ({0.9391*\dx},{-1.5445*\dy}) + -- ({0.8947*\dx},{-1.5316*\dy}) + -- ({0.8508*\dx},{-1.5173*\dy}) + -- ({0.8076*\dx},{-1.5017*\dy}) + -- ({0.7650*\dx},{-1.4848*\dy}) + -- ({0.7231*\dx},{-1.4666*\dy}) + -- ({0.6820*\dx},{-1.4471*\dy}) + -- ({0.6417*\dx},{-1.4263*\dy}) + -- ({0.6022*\dx},{-1.4043*\dy}) + -- ({0.5635*\dx},{-1.3811*\dy}) + -- ({0.5258*\dx},{-1.3568*\dy}) + -- ({0.4890*\dx},{-1.3313*\dy}) + -- ({0.4532*\dx},{-1.3048*\dy}) + -- ({0.4185*\dx},{-1.2771*\dy}) + -- ({0.3847*\dx},{-1.2485*\dy}) + -- ({0.3521*\dx},{-1.2188*\dy}) + -- ({0.3205*\dx},{-1.1882*\dy}) + -- ({0.2902*\dx},{-1.1567*\dy}) + -- ({0.2609*\dx},{-1.1243*\dy}) + -- ({0.2329*\dx},{-1.0911*\dy}) + -- ({0.2061*\dx},{-1.0571*\dy}) + -- ({0.1806*\dx},{-1.0224*\dy}) + -- ({0.1563*\dx},{-0.9870*\dy}) + -- ({0.1333*\dx},{-0.9509*\dy}) + -- ({0.1117*\dx},{-0.9142*\dy}) + -- ({0.0914*\dx},{-0.8769*\dy}) + -- ({0.0724*\dx},{-0.8391*\dy}) + -- ({0.0547*\dx},{-0.8008*\dy}) + -- ({0.0385*\dx},{-0.7622*\dy}) + -- ({0.0236*\dx},{-0.7231*\dy}) + -- ({0.0102*\dx},{-0.6837*\dy}) + -- ({-0.0019*\dx},{-0.6441*\dy}) + -- ({-0.0125*\dx},{-0.6042*\dy}) + -- ({-0.0217*\dx},{-0.5641*\dy}) + -- ({-0.0295*\dx},{-0.5239*\dy}) + -- ({-0.0359*\dx},{-0.4836*\dy}) + -- ({-0.0409*\dx},{-0.4433*\dy}) + -- ({-0.0444*\dx},{-0.4030*\dy}) + -- ({-0.0466*\dx},{-0.3628*\dy}) + -- ({-0.0473*\dx},{-0.3226*\dy}) + -- ({-0.0466*\dx},{-0.2827*\dy}) + -- ({-0.0445*\dx},{-0.2429*\dy}) + -- ({-0.0410*\dx},{-0.2034*\dy}) + -- ({-0.0362*\dx},{-0.1642*\dy}) + -- ({-0.0300*\dx},{-0.1254*\dy}) + -- ({-0.0224*\dx},{-0.0870*\dy}) + -- ({-0.0136*\dx},{-0.0490*\dy}) + -- ({-0.0034*\dx},{-0.0115*\dy}) + -- ({0.0081*\dx},{0.0255*\dy}) + -- ({0.0208*\dx},{0.0619*\dy}) + -- ({0.0348*\dx},{0.0976*\dy}) + -- ({0.0500*\dx},{0.1327*\dy}) + -- ({0.0663*\dx},{0.1671*\dy}) + -- ({0.0839*\dx},{0.2008*\dy}) + -- ({0.1026*\dx},{0.2336*\dy}) + -- ({0.1224*\dx},{0.2656*\dy}) + -- ({0.1432*\dx},{0.2968*\dy}) + -- ({0.1651*\dx},{0.3271*\dy}) + -- ({0.1880*\dx},{0.3564*\dy}) + -- ({0.2119*\dx},{0.3848*\dy}) + -- ({0.2367*\dx},{0.4122*\dy}) + -- ({0.2625*\dx},{0.4385*\dy}) + -- ({0.2890*\dx},{0.4638*\dy}) + -- ({0.3164*\dx},{0.4880*\dy}) + -- ({0.3446*\dx},{0.5111*\dy}) + -- ({0.3735*\dx},{0.5331*\dy}) + -- ({0.4031*\dx},{0.5539*\dy}) + -- ({0.4334*\dx},{0.5735*\dy}) + -- ({0.4643*\dx},{0.5919*\dy}) + -- ({0.4957*\dx},{0.6090*\dy}) + -- ({0.5276*\dx},{0.6250*\dy}) + -- ({0.5601*\dx},{0.6396*\dy}) + -- ({0.5929*\dx},{0.6530*\dy}) + -- ({0.6262*\dx},{0.6652*\dy}) + -- ({0.6597*\dx},{0.6760*\dy}) + -- ({0.6936*\dx},{0.6855*\dy}) + -- ({0.7277*\dx},{0.6937*\dy}) + -- ({0.7620*\dx},{0.7006*\dy}) + -- ({0.7964*\dx},{0.7062*\dy}) + -- ({0.8309*\dx},{0.7104*\dy}) + -- ({0.8655*\dx},{0.7133*\dy}) + -- ({0.9001*\dx},{0.7149*\dy}) + -- ({0.9346*\dx},{0.7152*\dy}) + -- ({0.9690*\dx},{0.7141*\dy}) + -- ({1.0033*\dx},{0.7117*\dy}) + -- ({1.0374*\dx},{0.7081*\dy}) + -- ({1.0712*\dx},{0.7031*\dy}) + -- ({1.1048*\dx},{0.6969*\dy}) + -- ({1.1380*\dx},{0.6894*\dy}) + -- ({1.1709*\dx},{0.6806*\dy}) + -- ({1.2033*\dx},{0.6706*\dy}) + -- ({1.2353*\dx},{0.6594*\dy}) + -- ({1.2667*\dx},{0.6470*\dy}) + -- ({1.2976*\dx},{0.6334*\dy}) + -- ({1.3279*\dx},{0.6186*\dy}) + -- ({1.3576*\dx},{0.6027*\dy}) + -- ({1.3866*\dx},{0.5857*\dy}) + -- ({1.4149*\dx},{0.5676*\dy}) + -- ({1.4424*\dx},{0.5485*\dy}) + -- ({1.4692*\dx},{0.5284*\dy}) + -- ({1.4951*\dx},{0.5072*\dy}) + -- ({1.5201*\dx},{0.4851*\dy}) + -- ({1.5443*\dx},{0.4621*\dy}) + -- ({1.5675*\dx},{0.4381*\dy}) + -- ({1.5898*\dx},{0.4133*\dy}) + -- ({1.6111*\dx},{0.3877*\dy}) + -- ({1.6314*\dx},{0.3614*\dy}) + -- ({1.6506*\dx},{0.3342*\dy}) + -- ({1.6687*\dx},{0.3064*\dy}) + -- ({1.6858*\dx},{0.2779*\dy}) + -- ({1.7017*\dx},{0.2488*\dy}) + -- ({1.7165*\dx},{0.2191*\dy}) + -- ({1.7302*\dx},{0.1889*\dy}) + -- ({1.7427*\dx},{0.1581*\dy}) + -- ({1.7540*\dx},{0.1270*\dy}) + -- ({1.7640*\dx},{0.0954*\dy}) + -- ({1.7729*\dx},{0.0635*\dy}) + -- ({1.7806*\dx},{0.0312*\dy}) + -- ({1.7870*\dx},{-0.0013*\dy}) + -- ({1.7921*\dx},{-0.0340*\dy}) + -- ({1.7960*\dx},{-0.0669*\dy}) + -- ({1.7987*\dx},{-0.1000*\dy}) + -- ({1.8000*\dx},{-0.1331*\dy}) + -- ({1.8002*\dx},{-0.1662*\dy}) + -- ({1.7990*\dx},{-0.1993*\dy}) + -- ({1.7967*\dx},{-0.2324*\dy}) + -- ({1.7930*\dx},{-0.2654*\dy}) + -- ({1.7881*\dx},{-0.2982*\dy}) + -- ({1.7820*\dx},{-0.3308*\dy}) + -- ({1.7747*\dx},{-0.3632*\dy}) + -- ({1.7661*\dx},{-0.3952*\dy}) + -- ({1.7563*\dx},{-0.4270*\dy}) + -- ({1.7454*\dx},{-0.4584*\dy}) + -- ({1.7332*\dx},{-0.4893*\dy}) + -- ({1.7199*\dx},{-0.5198*\dy}) + -- ({1.7055*\dx},{-0.5497*\dy}) + -- ({1.6900*\dx},{-0.5792*\dy}) + -- ({1.6733*\dx},{-0.6080*\dy}) + -- ({1.6556*\dx},{-0.6362*\dy}) + -- ({1.6368*\dx},{-0.6637*\dy}) + -- ({1.6171*\dx},{-0.6906*\dy}) + -- ({1.5963*\dx},{-0.7166*\dy}) + -- ({1.5746*\dx},{-0.7419*\dy}) + -- ({1.5519*\dx},{-0.7664*\dy}) + -- ({1.5283*\dx},{-0.7901*\dy}) + -- ({1.5039*\dx},{-0.8128*\dy}) + -- ({1.4787*\dx},{-0.8347*\dy}) + -- ({1.4526*\dx},{-0.8556*\dy}) + -- ({1.4258*\dx},{-0.8756*\dy}) + -- ({1.3983*\dx},{-0.8945*\dy}) + -- ({1.3700*\dx},{-0.9124*\dy}) + -- ({1.3412*\dx},{-0.9293*\dy}) + -- ({1.3117*\dx},{-0.9452*\dy}) + -- ({1.2817*\dx},{-0.9599*\dy}) + -- ({1.2511*\dx},{-0.9735*\dy}) + -- ({1.2201*\dx},{-0.9860*\dy}) + -- ({1.1886*\dx},{-0.9974*\dy}) + -- ({1.1567*\dx},{-1.0076*\dy}) + -- ({1.1245*\dx},{-1.0166*\dy}) + -- ({1.0920*\dx},{-1.0245*\dy}) + -- ({1.0592*\dx},{-1.0312*\dy}) + -- ({1.0262*\dx},{-1.0367*\dy}) + -- ({0.9931*\dx},{-1.0409*\dy}) + -- ({0.9598*\dx},{-1.0440*\dy}) + -- ({0.9264*\dx},{-1.0459*\dy}) + -- ({0.8930*\dx},{-1.0465*\dy}) + -- ({0.8596*\dx},{-1.0460*\dy}) + -- ({0.8263*\dx},{-1.0442*\dy}) + -- ({0.7930*\dx},{-1.0413*\dy}) +} diff --git a/buch/papers/zeta/images/zetaplot.m b/buch/papers/zeta/images/zetaplot.m new file mode 100644 index 0000000..984b645 --- /dev/null +++ b/buch/papers/zeta/images/zetaplot.m @@ -0,0 +1,23 @@ +% +% zetaplot.m +% +% (c) 2022 Prof Dr Andreas Müller +% +s = 1; +h = 0.02; +m = 40; + +fn = fopen("zetapath.tex", "w"); +fprintf(fn, "\\def\\zetapath{\n"); +counter = 0; +for y = (0:h:m) + if (counter > 0) + fprintf(fn, "\n\t--"); + end + z = zeta(0.5 + i*y); + fprintf(fn, " ({%.4f*\\dx},{%.4f*\\dy})", real(z), imag(z)); + counter = counter + 1; +end +fprintf(fn, "\n}\n"); +fclose(fn); + diff --git a/buch/papers/zeta/images/zetaplot.pdf b/buch/papers/zeta/images/zetaplot.pdf Binary files differnew file mode 100644 index 0000000..c6d3693 --- /dev/null +++ b/buch/papers/zeta/images/zetaplot.pdf diff --git a/buch/papers/zeta/images/zetaplot.tex b/buch/papers/zeta/images/zetaplot.tex new file mode 100644 index 0000000..521bb1a --- /dev/null +++ b/buch/papers/zeta/images/zetaplot.tex @@ -0,0 +1,47 @@ +% +% zetaplot.tex -- Abbildung der kritischen Geraden +% +% (c) 2021 Prof Dr Andreas Müller, OST Ostschweizer Fachhochschule +% +\documentclass[tikz]{standalone} +\usepackage{amsmath} +\usepackage{times} +\usepackage{txfonts} +\usepackage{pgfplots} +\usepackage{csvsimple} +\usetikzlibrary{arrows,intersections,math} +\begin{document} +\def\skala{1} +\begin{tikzpicture}[>=latex,thick,scale=\skala] + +\def\dx{2} +\def\dy{2} + +\draw[->] ({-1.6*\dx},0) -- ({3.4*\dx},0) + coordinate[label={$\Re\zeta(\frac12+it)$}]; +\draw[->] (0,{-2.1*\dx}) -- (0,{2.2*\dx}) + coordinate[label={left:$\Im\zeta(\frac12+it)$}]; + +\foreach \x in {-1,1,2,3}{ + \node at ({\x*\dx},-0.1) [below] {$\x$}; +} +\node at (-0.1,{1*\dy}) [above left] {$i$}; +\node at (-0.1,{2*\dy}) [left] {$2i$}; +\node at (-0.1,{-1*\dy}) [below left] {$-i$}; +\node at (-0.1,{-2*\dy}) [left] {$-2i$}; + +\foreach \x in {-1,1,2,3}{ + \draw ({\x*\dx},-0.1) -- ({\x*\dx},0.1); +} +\foreach \y in {1,2}{ + \draw (-0.1,{\y*\dy}) -- (0.1,{\y*\dy}); + \draw (-0.1,{-\y*\dy}) -- (0.1,{-\y*\dy}); +} + +\input{papers/zeta/images/zetapath.tex} + +\draw[color=blue,line width=1pt] \zetapath; + +\end{tikzpicture} +\end{document} + diff --git a/buch/papers/zeta/main.tex b/buch/papers/zeta/main.tex index caddace..de297a0 100644 --- a/buch/papers/zeta/main.tex +++ b/buch/papers/zeta/main.tex @@ -8,12 +8,12 @@ \begin{refsection} \chapterauthor{Raphael Unterer} -%TODO Einleitung \input{papers/zeta/einleitung.tex} \input{papers/zeta/euler_product.tex} \input{papers/zeta/zeta_gamma.tex} \input{papers/zeta/analytic_continuation.tex} +\input{papers/zeta/fazit} \printbibliography[heading=subbibliography] \end{refsection} diff --git a/buch/papers/zeta/presentation/presentation.tex b/buch/papers/zeta/presentation/presentation.tex new file mode 100644 index 0000000..53fd305 --- /dev/null +++ b/buch/papers/zeta/presentation/presentation.tex @@ -0,0 +1,368 @@ +\documentclass[ngerman, aspectratio=169]{beamer} + +%style +\mode<presentation>{ + \usetheme{Frankfurt} +} +%packages +\usepackage[utf8]{inputenc} +\usepackage[english]{babel} +\usepackage{graphicx} +\usepackage{array} + +\newcolumntype{L}[1]{>{\raggedright\let\newline\\\arraybackslash\hspace{0pt}}m{#1}} +\usepackage{ragged2e} + +\usepackage{bm} % bold math +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{mathtools} +\usepackage{amsmath} +\usepackage{multirow} % multi row in tables +\usepackage{scrextend} + +\usepackage{tikz} + +\usepackage{algorithmic} + +%\usepackage{algorithm} % http://ctan.org/pkg/algorithm +%\usepackage{algpseudocode} % http://ctan.org/pkg/algorithmicx + +%\usepackage{algorithmicx} + + +%citations +\usepackage[style=verbose,backend=biber]{biblatex} +\addbibresource{references.bib} + + + +\usefonttheme[onlymath]{serif} + +%Beamer Template modifications +%\definecolor{mainColor}{HTML}{0065A3} % HSR blue +\definecolor{mainColor}{HTML}{D72864} % OST pink +\definecolor{invColor}{HTML}{28d79b} % OST pink +\definecolor{dgreen}{HTML}{38ad36} % Dark green + +%\definecolor{mainColor}{HTML}{000000} % HSR blue +\setbeamercolor{palette primary}{bg=white,fg=mainColor} +\setbeamercolor{palette secondary}{bg=orange,fg=mainColor} +\setbeamercolor{palette tertiary}{bg=yellow,fg=red} +\setbeamercolor{palette quaternary}{bg=mainColor,fg=white} %bg = Top bar, fg = active top bar topic +\setbeamercolor{structure}{fg=black} % itemize, enumerate, etc (bullet points) +\setbeamercolor{section in toc}{fg=black} % TOC sections +\setbeamertemplate{section in toc}[sections numbered] +\setbeamertemplate{subsection in toc}{% + \hspace{1.2em}{$\bullet$}~\inserttocsubsection\par} + +\setbeamertemplate{itemize items}[circle] +\setbeamertemplate{description item}[circle] +\setbeamertemplate{title page}[default][colsep=-4bp,rounded=true] +\beamertemplatenavigationsymbolsempty + +\setbeamercolor{footline}{fg=gray} +\setbeamertemplate{footline}{% + \hfill\usebeamertemplate***{navigation symbols} + \hspace{0.5cm} + \insertframenumber{}\hspace{0.2cm}\vspace{0.2cm} +} + +\usepackage{caption} +\captionsetup{labelformat=empty} + +%Title Page +\title{Riemannsche Zeta Funktion} +\author{Raphael Unterer} +\institute{Mathematisches Seminar 2022: Spezielle Funktionen} + +\newcommand*{\HL}{\textcolor{mainColor}} +\newcommand*{\RD}{\textcolor{red}} +\newcommand*{\BL}{\textcolor{blue}} +\newcommand*{\GN}{\textcolor{dgreen}} +\newcommand*{\YE}{\textcolor{violet}} + + + + +\makeatletter +\newcount\my@repeat@count +\newcommand{\myrepeat}[2]{% + \begingroup + \my@repeat@count=\z@ + \@whilenum\my@repeat@count<#1\do{#2\advance\my@repeat@count\@ne}% + \endgroup +} +\makeatother + + + + +\usetikzlibrary{automata,arrows,positioning,calc} + + +\begin{document} + + %Titelseite + \begin{frame} + \titlepage + \end{frame} + + %Inhaltsverzeichnis +% \begin{frame} +% \frametitle{Inhalt} +% \tableofcontents +% \end{frame} + + \section{Motivation} + + \begin{frame} + \frametitle{Summe aller Natürlichen Zahlen} + \begin{equation*} + \sum_{n=1}^{\infty} n + = + 1 + 2 + 3 + \ldots + \infty + = + - \frac{1}{12} + \end{equation*} + \end{frame} + \begin{frame} + \frametitle{Summe aller Natürlichen Zahlen} + \begin{center} + \includegraphics[width=0.7\textwidth]{../images/youtube_screenshot.png} + \end{center} + \end{frame} + \begin{frame} + \frametitle{Riemannsche Zeta Funktion} + \begin{equation*} + \zeta(s) + = + \sum_{n=1}^{\infty} + \frac{1}{n^s} + \end{equation*} + \pause + \begin{equation*} + \zeta(-1) + = + \sum_{n=1}^{\infty} + \frac{1}{n^{-1}} + = + \sum_{n=1}^{\infty} n + \end{equation*} + \end{frame} + \begin{frame} + \frametitle{Originaler Definitionsbereich} + Wir kennen die divergierende harmonische Reihe + \begin{equation*} + \zeta(1) + = + \sum_{n=1}^{\infty} + \frac{1}{n} + \rightarrow + \infty, + \end{equation*} + und somit ist $\Re(s) > 1$. + \end{frame} + + \section{Analytische Fortsetzung} + \begin{frame} + \frametitle{Plan für die Analytische Fortsetzung von $\zeta(s)$} + \begin{center} + \input{../images/continuation_overview.tikz.tex} + \end{center} + \end{frame} + \begin{frame} + \frametitle{Fortsetzung auf $\Re(s) > 0$} + Dirichletsche Etafunktion ist + \begin{equation*}\label{zeta:equation:eta} + \eta(s) + = + \sum_{n=1}^{\infty} + \frac{(-1)^{n-1}}{n^s}, + \end{equation*} + und konvergiert im Bereich $\Re(s) > 0$. + \end{frame} + \begin{frame} + \frametitle{Fortsetzung auf $\Re(s) > 0$} + \begin{align} + \zeta(s) + &= + \RD{ + \sum_{n=1}^{\infty} + \frac{1}{n^s} \label{zeta:align1} + } + \\ + \frac{1}{2^{s-1}} + \zeta(s) + &= + \BL{ + \sum_{n=1}^{\infty} + \frac{2}{(2n)^s} \label{zeta:align2} + } + \end{align} + \pause + \eqref{zeta:align1} - \eqref{zeta:align2}: + \begin{align*} + \left(1 - \frac{1}{2^{s-1}} \right) + \zeta(s) + &= + \RD{\frac{1}{1^s}} + \underbrace{-\BL{\frac{2}{2^s}} + \RD{\frac{1}{2^s}}}_{-\frac{1}{2^s}} + + \RD{\frac{1}{3^s}} + \underbrace{-\BL{\frac{2}{4^s}} + \RD{\frac{1}{4^s}}}_{-\frac{1}{4^s}} + \ldots + \\ + &= \eta(s) + \end{align*} + \end{frame} + \begin{frame} + \frametitle{Fortsetzung auf $\Re(s) > 0$} + Somit haben wir die Fortsetzung gefunden als + \begin{equation} \label{zeta:equation:fortsetzung1} + \zeta(s) + := + \left(1 - \frac{1}{2^{s-1}} \right)^{-1} \eta(s). + \end{equation} + \end{frame} + \begin{frame} + \frametitle{Spiegelungseigenschaft für $\Re(s) < 0$} + \begin{equation*}\label{zeta:equation:functional} + \frac{\Gamma \left( \frac{s}{2} \right)}{\pi^{\frac{s}{2}}} + \zeta(s) + = + \frac{\Gamma \left( \frac{1-s}{2} \right)}{\pi^{\frac{1-s}{2}}} + \zeta(1-s). + \end{equation*} + \end{frame} + %TODO maybe explain gamma-fct + + \section{Euler Produkt und Primzahlen} + \begin{frame} + \frametitle{Wieso ist die Zeta Funktion so bekannt?} + \begin{itemize} + \item Interessante Funktionswerte z.B. $\zeta(2) = \frac{\pi^2}{6}$ + \item Primzahlenverteilung (Riemannhypothese) + \item Forschungsgebiet der analytischen Zahlentheorie seit dem 18. Jahrhundert + \item ... + \end{itemize} + \end{frame} + \begin{frame} + \frametitle{Euler Produkt: Verbindung von Zeta und Primzahlen} + \begin{equation*} + \zeta(s) + = + \sum_{n=1}^\infty + \frac{1}{n^s} + = + \prod_{p \in P} + \frac{1}{1-p^{-s}} + \end{equation*} + \pause + Geometrische Reihe + \begin{equation*} + \prod_{p \in P} + \frac{1}{1-p^{-s}} + = + \prod_{p \in P} + \left( + 1 + + + \frac{1}{p^s} + + + \frac{1}{p^{2s}} + + + \frac{1}{p^{3s}} + + + \ldots + \right) + \end{equation*} + \pause + Erste Terme ausmultiplizieren + \begin{align*} + \left( + 1 + + + \RD{\frac{1}{2^s}} + + + \GN{\frac{1}{2^{2s}}} + + + \frac{1}{2^{3s}} + + + \ldots + \right) + \left( + 1 + + + \BL{\frac{1}{3^s}} + + + \frac{1}{3^{2s}} + + + \frac{1}{3^{3s}} + + + \ldots + \right) + \left( + 1 + + + \YE{\frac{1}{5^s}} + + + \frac{1}{5^{2s}} + + + \frac{1}{5^{3s}} + + + \ldots + \right) + \ldots + \\ + = + 1 + + + \RD{\frac{1}{2^s}} + + + \BL{\frac{1}{3^s}} + + + \GN{\frac{1}{4^s}} + + + \YE{\frac{1}{5^s}} + + + \ldots + \end{align*} + \end{frame} + \begin{frame} + \frametitle{Primzahlfunktion} + \begin{center} + \scalebox{0.5}{\input{../images/primzahlfunktion.pgf}} + \end{center} + \end{frame} + + + \section{Darstellungen} + + \begin{frame} + \frametitle{Farbcodierung} + \begin{center} + \scalebox{0.6}{\input{zeta_color_plot.pgf}} + \end{center} + \end{frame} + + \begin{frame} + \frametitle{Konstanter Realteil $\Re(s)=-1$ und $\Im(s)=0\ldots40$} + \begin{center} + \scalebox{0.6}{\input{../images/zeta_re_-1_plot.pgf}} + \end{center} + \end{frame} + \begin{frame} + \frametitle{Konstanter Realteil $\Re(s)=0$ und $\Im(s)=0\ldots40$} + \begin{center} + \scalebox{0.6}{\input{../images/zeta_re_0_plot.pgf}} + \end{center} + \end{frame} + \begin{frame} + \frametitle{Konstanter Realteil $\Re(s)=0.5$ und $\Im(s)=0\ldots40$} + \begin{center} + \scalebox{0.6}{\input{../images/zeta_re_0.5_plot.pgf}} + \end{center} + \end{frame} + +\end{document} + diff --git a/buch/papers/zeta/presentation/zeta_color_plot-img0.png b/buch/papers/zeta/presentation/zeta_color_plot-img0.png Binary files differnew file mode 100644 index 0000000..b8c7298 --- /dev/null +++ b/buch/papers/zeta/presentation/zeta_color_plot-img0.png diff --git a/buch/papers/zeta/presentation/zeta_color_plot.pgf b/buch/papers/zeta/presentation/zeta_color_plot.pgf new file mode 100644 index 0000000..0fd7cb8 --- /dev/null +++ b/buch/papers/zeta/presentation/zeta_color_plot.pgf @@ -0,0 +1,402 @@ +%% Creator: Matplotlib, PGF backend +%% +%% To include the figure in your LaTeX document, write +%% \input{<filename>.pgf} +%% +%% Make sure the required packages are loaded in your preamble +%% \usepackage{pgf} +%% +%% and, on pdftex +%% \usepackage[utf8]{inputenc}\DeclareUnicodeCharacter{2212}{-} +%% +%% or, on luatex and xetex +%% \usepackage{unicode-math} +%% +%% Figures using additional raster images can only be included by \input if +%% they are in the same directory as the main LaTeX file. For loading figures +%% from other directories you can use the `import` package +%% \usepackage{import} +%% +%% and then include the figures with +%% \import{<path to file>}{<filename>.pgf} +%% +%% Matplotlib used the following preamble +%% +\begingroup% +\makeatletter% +\begin{pgfpicture}% +\pgfpathrectangle{\pgfpointorigin}{\pgfqpoint{6.400000in}{4.800000in}}% +\pgfusepath{use as bounding box, clip}% +\begin{pgfscope}% +\pgfsetbuttcap% +\pgfsetmiterjoin% +\definecolor{currentfill}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetfillcolor{currentfill}% +\pgfsetlinewidth{0.000000pt}% +\definecolor{currentstroke}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetstrokecolor{currentstroke}% +\pgfsetdash{}{0pt}% +\pgfpathmoveto{\pgfqpoint{0.000000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{6.400000in}{0.000000in}}% +\pgfpathlineto{\pgfqpoint{6.400000in}{4.800000in}}% +\pgfpathlineto{\pgfqpoint{0.000000in}{4.800000in}}% +\pgfpathclose% +\pgfusepath{fill}% +\end{pgfscope}% +\begin{pgfscope}% +\pgfsetbuttcap% +\pgfsetmiterjoin% +\definecolor{currentfill}{rgb}{1.000000,1.000000,1.000000}% +\pgfsetfillcolor{currentfill}% +\pgfsetlinewidth{0.000000pt}% +\definecolor{currentstroke}{rgb}{0.000000,0.000000,0.000000}% +\pgfsetstrokecolor{currentstroke}% +\pgfsetstrokeopacity{0.000000}% +\pgfsetdash{}{0pt}% +\pgfpathmoveto{\pgfqpoint{2.588156in}{0.528000in}}% +\pgfpathlineto{\pgfqpoint{3.971844in}{0.528000in}}% +\pgfpathlineto{\pgfqpoint{3.971844in}{4.224000in}}% +\pgfpathlineto{\pgfqpoint{2.588156in}{4.224000in}}% +\pgfpathclose% +\pgfusepath{fill}% +\end{pgfscope}% +\begin{pgfscope}% +\pgfpathrectangle{\pgfqpoint{2.588156in}{0.528000in}}{\pgfqpoint{1.383688in}{3.696000in}}% +\pgfusepath{clip}% +\pgfsys@transformshift{2.588156in}{0.528000in}% +\pgftext[left,bottom]{\includegraphics[interpolate=true,width=1.390000in,height=3.700000in]{zeta_color_plot-img0.png}}% +\end{pgfscope}% +\begin{pgfscope}% +\pgfsetbuttcap% +\pgfsetroundjoin% 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+\endgroup% diff --git a/buch/papers/zeta/python/plot_zeta.py b/buch/papers/zeta/python/plot_zeta.py new file mode 100644 index 0000000..53097c5 --- /dev/null +++ b/buch/papers/zeta/python/plot_zeta.py @@ -0,0 +1,39 @@ +import numpy as np +from mpmath import zeta +import matplotlib.pyplot as plt +from matplotlib import colors +import matplotlib +matplotlib.use("pgf") +matplotlib.rcParams.update( + { + "pgf.texsystem": "pdflatex", + "font.family": "serif", + "font.size": 8, + "text.usetex": True, + "pgf.rcfonts": False, + "axes.unicode_minus": False, + } +) + +print(zeta(-1)) +print(zeta(-1 + 2j)) + +re_values = np.arange(-10, 5, 0.04) +im_values = np.arange(-20, 20, 0.04) +plot_matrix = np.zeros((len(im_values), len(re_values), 3)) +for im_i, im in enumerate(im_values): + print(im_i) + for re_i, re in enumerate(re_values): + z = complex(zeta(re + 1j*im)) + h = (np.angle(z) + np.pi) / (2*np.pi) + v = np.abs(z) + s = 1.0 + plot_matrix[im_i, re_i] = [h, s, v] + +log10_v = np.log10(plot_matrix[:, :, 2]) +log10_v += np.abs(np.min(log10_v)) +plot_matrix[:, :, 2] = (log10_v) / np.max(log10_v) +plt.imshow(colors.hsv_to_rgb(plot_matrix), extent=[re_values.min(), re_values.max(), im_values.min(), im_values.max()]) +plt.xlabel("$\Re$") +plt.ylabel("$\Im$") +plt.savefig(f"zeta_color_plot.pgf") diff --git a/buch/papers/zeta/python/plot_zeta2.py b/buch/papers/zeta/python/plot_zeta2.py new file mode 100644 index 0000000..b730703 --- /dev/null +++ b/buch/papers/zeta/python/plot_zeta2.py @@ -0,0 +1,31 @@ +import numpy as np +from mpmath import zeta +import matplotlib.pyplot as plt +import matplotlib +matplotlib.use("pgf") +matplotlib.rcParams.update( + { + "pgf.texsystem": "pdflatex", + "font.family": "serif", + "font.size": 8, + "text.usetex": True, + "pgf.rcfonts": False, + "axes.unicode_minus": False, + } +) +# const re plot +re_values = [-1, 0, 0.5] +im_values = np.arange(0, 40, 0.04) +buf = np.zeros((len(re_values), len(im_values), 2)) +for im_i, im in enumerate(im_values): + print(im_i) + for re_i, re in enumerate(re_values): + z = complex(zeta(re + 1j*im)) + buf[re_i, im_i] = [np.real(z), np.imag(z)] + +for i in range(len(re_values)): + plt.figure() + plt.plot(buf[i,:,0], buf[i,:,1], label=f"$\Re={re_values[i]}$") + plt.xlabel("$\Re$") + plt.ylabel("$\Im$") + plt.savefig(f"zeta_re_{re_values[i]}_plot.pgf") diff --git a/buch/papers/zeta/python/primzahlfunktion.py b/buch/papers/zeta/python/primzahlfunktion.py new file mode 100644 index 0000000..9434de9 --- /dev/null +++ b/buch/papers/zeta/python/primzahlfunktion.py @@ -0,0 +1,24 @@ +import matplotlib.pyplot as plt +import numpy as np + +primzahlfunktion = [0, 0, 0, 0] +x = [0, 1-1e-12, 1, 2-1e-12] +x_last = 1 +value = 0 +for i in range(2, 30, 1): + new_value = value + 1 + for j in range(2, i, 1): + if i % j == 0: + new_value = value + value = new_value + primzahlfunktion.append(new_value) + x_last += 1 + x.append(x_last) + primzahlfunktion.append(new_value) + x.append(x_last + 1 - 1e-12) + + +plt.rcParams.update({"pgf.texsystem": "pdflatex"}) +plt.plot(x, primzahlfunktion) +plt.show() + diff --git a/buch/papers/zeta/references.bib b/buch/papers/zeta/references.bib index a4f2521..f2a2f31 100644 --- a/buch/papers/zeta/references.bib +++ b/buch/papers/zeta/references.bib @@ -4,32 +4,58 @@ % (c) 2020 Autor, Hochschule Rapperswil % -@online{zeta:bibtex, - title = {BibTeX}, - url = {https://de.wikipedia.org/wiki/BibTeX}, - date = {2020-02-06}, - year = {2020}, - month = {2}, - day = {6} +@online{zeta:online:millennium, + title = {The Millennium Prize Problems}, + url = {https://www.claymath.org/millennium-problems/millennium-prize-problems}, + year = {2022}, + month = {8}, + day = {4} } -@book{zeta:numerical-analysis, - title = {Numerical Analysis}, - author = {David Kincaid and Ward Cheney}, - publisher = {American Mathematical Society}, - year = {2002}, - isbn = {978-8-8218-4788-6}, - inseries = {Pure and applied undegraduate texts}, - volume = {2} +@online{zeta:online:wiki_en, + title = {Riemann zeta function}, + url = {https://en.wikipedia.org/wiki/Riemann_zeta_function}, + year = {2022}, + month = {8}, + day = {7} +} +@online{zeta:online:wiki_de, + title = {Riemannsche Zeta-Funktion}, + url = {https://de.wikipedia.org/wiki/Riemannsche_Zeta-Funktion}, + year = {2022}, + month = {8}, + day = {7} +} + +@online{zeta:online:poisson, + title = {Deriving the Poisson Summation Formula}, + url = {https://www.youtube.com/watch?v=4Bex-4BFYWo}, + author = {Physics and Math Lectures}, + year = {2022}, + month = {8}, + day = {7} } -@article{zeta:mendezmueller, - author = { Tabea Méndez and Andreas Müller }, - title = { Noncommutative harmonic analysis and image registration }, - journal = { Appl. Comput. Harmon. Anal.}, - year = 2019, - volume = 47, - pages = {607--627}, - url = {https://doi.org/10.1016/j.acha.2017.11.004} +@online{zeta:online:mryoumath, + title = {Riemann Zeta Function Playlist}, + url = {https://www.youtube.com/playlist?list=PL32446FDD4DA932C9}, + author = {MrYouMath}, + year = {2022}, + month = {8}, + day = {7} } +@online{zeta:online:basel, + title = {Basel Problem}, + url = {https://en.wikipedia.org/wiki/Basel_problem}, + year = {2022}, + month = {8}, + day = {7} +} +@online{zeta:online:pars, + title = {Parseval's identity}, + url = {https://en.wikipedia.org/wiki/Parseval%27s_identity}, + year = {2022}, + month = {8}, + day = {7} +} diff --git a/buch/papers/zeta/zeta_color_plot-img0.png b/buch/papers/zeta/zeta_color_plot-img0.png Binary files differnew file mode 100644 index 0000000..b8c7298 --- /dev/null +++ b/buch/papers/zeta/zeta_color_plot-img0.png diff --git a/buch/papers/zeta/zeta_color_plot.pgf b/buch/papers/zeta/zeta_color_plot.pgf new file mode 100644 index 0000000..0fd7cb8 --- /dev/null +++ b/buch/papers/zeta/zeta_color_plot.pgf @@ -0,0 +1,402 @@ +%% Creator: Matplotlib, PGF backend +%% +%% To include the figure in your LaTeX document, write +%% \input{<filename>.pgf} +%% +%% Make sure the required packages are loaded in your preamble +%% \usepackage{pgf} +%% +%% and, on pdftex +%% \usepackage[utf8]{inputenc}\DeclareUnicodeCharacter{2212}{-} +%% +%% or, on luatex and xetex +%% \usepackage{unicode-math} +%% +%% Figures using additional raster images can only be included by \input if +%% they are in the same directory as the main LaTeX file. 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+\endgroup% diff --git a/buch/papers/zeta/zeta_gamma.tex b/buch/papers/zeta/zeta_gamma.tex index db41676..dd422e3 100644 --- a/buch/papers/zeta/zeta_gamma.tex +++ b/buch/papers/zeta/zeta_gamma.tex @@ -11,7 +11,7 @@ Wir erinnern uns an die Definition der Gammafunktion in \eqref{buch:rekursion:ga \int_0^{\infty} t^{s-1} e^{-t} \,dt, \end{equation*} wobei die Notation an die Zetafunktion angepasst ist. -Durch die Substitution von $t$ mit $t = nu$ und $dt = n\,du$ wird daraus +Durch die Substitution $t = nu$ und $dt = n\,du$ wird daraus \begin{align*} \Gamma(s) &= @@ -19,7 +19,7 @@ Durch die Substitution von $t$ mit $t = nu$ und $dt = n\,du$ wird daraus &= \int_0^{\infty} n^s u^{s-1} e^{-nu} \,du. \end{align*} -Durch Division mit durch $n^s$ ergibt sich die Quotienten +Durch Division durch $n^s$ ergeben sich die Quotienten \begin{equation*} \frac{\Gamma(s)}{n^s} = @@ -57,5 +57,5 @@ Wenn wir dieses Resultat einsetzen in \eqref{zeta:equation:zeta_gamma1} und durc \frac{1}{\Gamma(s)} \int_0^{\infty} \frac{u^{s-1}}{e^u -1} - du \qed + du. \end{equation} |
