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| \documentclass[uebung]{lecture} | |||||
| \title{Wtheo 0: Übungsblatt 9} | |||||
| \author{Josua Kugler, Christian Merten} | |||||
| \newcommand{\E}{\mathbb{E}} | |||||
| \usepackage[]{mathrsfs} | |||||
| \newcommand{\cov}{\mathbb{C}\text{ov}} | |||||
| \newcommand{\var}{\mathbb{V}\text{ar}} | |||||
| \newcommand{\tageq}{\stepcounter{equation}\tag{\theequation}} | |||||
| \newcommand{\indep}{\perp \!\!\! \perp} | |||||
| \begin{document} | |||||
| \punkte[33] | |||||
| \begin{aufgabe} | |||||
| \begin{enumerate}[(a)] | |||||
| \item Anwenden der Formel der VL ergibt sofort für $x \in \R$: | |||||
| \begin{salign*} | |||||
| f^{X}(x) &= \int_{\R}^{} f^{X,Y}(x,y) \d{y} \\ | |||||
| &= \int_{\R}^{} \frac{1}{\pi} \mathbbm{1}_{\{(x,y) \in E\} } \d{y} \\ | |||||
| &= \mathbbm{1}_{\{|x| \le 1\}} \int_{-\sqrt{1-x^2} }^{\sqrt{1-x^2} } \frac{1}{\pi} \d{y} \\ | |||||
| &= \frac{2}{\pi} \sqrt{1-x^2} \mathbbm{1}_{\{|x| \le 1\}} | |||||
| \intertext{ | |||||
| Ganz analog folgt für $y \in \R$:} | |||||
| f^{Y}(y) &= \frac{2}{\pi} \sqrt{1-y^2} \mathbbm{1}_{\{|y| \le 1\} } | |||||
| .\end{salign*} | |||||
| \item Anwenden der Formel der VL ergibt zunächst mit Anwendung des Transformationssatzes | |||||
| \begin{salign*} | |||||
| \E(X) &= \int_{\R}^{} x f^{X}(x) \d{x} \\ | |||||
| &= \frac{1}{\pi} \int_{-1}^{1} 2x \sqrt{1-x^2} \d{x} \\ | |||||
| &= \frac{1}{\pi} \left[ \int_{-1}^{0} 2x \sqrt{1-x^2} \d{x} | |||||
| + \int_{0}^{1} 2x \sqrt{1-x^2} \d{x} \right] \\ | |||||
| &\stackrel{z = 1-x^2}{=} \frac{1}{\pi} \left[ \int_{0}^{1} - \sqrt{z} \d{z} | |||||
| + \int_{1}^{0} - \sqrt{z} \d{z} \right] \\ | |||||
| &= 0 | |||||
| \intertext{Unter erneuter Formelanwendung folgt} | |||||
| \E(X^2) &= \int_{\R}^{} x^2 f^{X}(x) \d{x} \\ | |||||
| &= \frac{2}{\pi} \int_{-1}^{1} x^2 \sqrt{1-x^2} \d{x} \\ | |||||
| &\stackrel{x = \sin(\varphi)}{=} \frac{2}{\pi} \int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} | |||||
| \sin^2(\varphi) \cos^2(\varphi)\d{\varphi} \\ | |||||
| &= \frac{2}{\pi} \int_{-\frac{\pi}{2}}^{\frac{\pi}{2}} \frac{1}{4} \sin^2(2\varphi) \d{\varphi} \\ | |||||
| &\stackrel{\psi = 2 \varphi}{=} | |||||
| \frac{1}{2\pi} \int_{-\pi}^{\pi} \sin^2(\psi) \frac{1}{2} \d{\psi} \\ | |||||
| &= \frac{1}{4 \pi} \int_{-\pi}^{\pi} \frac{1}{2}(\sin^2(\psi) + \cos^2(\psi)) \d{\psi} \\ | |||||
| &= \frac{1}{8 \pi} 2 \pi \\ | |||||
| &= \frac{1}{4} | |||||
| \intertext{Damit folgt} | |||||
| \var(X) &= \frac{1}{4} | |||||
| \intertext{Ganz analog} | |||||
| \var(Y) &= \frac{1}{4} | |||||
| \intertext{Betrachte nun zunächst} | |||||
| \int_{0}^{2\pi} \sin(\varphi) \cos(\varphi)\d{\varphi} | |||||
| &\stackrel{\text{part. Integrat.}}{=} \underbrace{\sin^2\varphi \Big|_{0}^{2\pi}}_{= 0} | |||||
| - \int_{0}^{2\pi} \sin\varphi \cos\varphi \d{\varphi} \\ | |||||
| \intertext{Damit folgt} | |||||
| \int_{0}^{2\pi} \sin\varphi \cos\varphi \d{\varphi} &= 0 | |||||
| \tageq \label{eq:1} | |||||
| \intertext{Es ist $\int_{\R^2}^{} \left|\frac{xy}{\pi} \right| \mathbbm{1}_{\{(x,y) \in E\}} | |||||
| \d{(x,y)} \le \frac{1}{\pi}\mathscr{L}^{2}(E) = 1 < \infty$, | |||||
| d.h. Fubini ist anwendbar. Damit folgt} | |||||
| \E(XY) &= \int_{\R^2}^{} xy f^{X,Y}(x,y) \d{(x,y)} \\ | |||||
| &= \int_{\R}^{} \int_{\R}^{} \frac{xy}{\pi} \mathbbm{1}_{\{(x,y) \in E\} } \d{x} \d{y} \\ | |||||
| &\stackrel{\text{Trafosatz}}{=} | |||||
| \frac{1}{\pi}\int_{0}^{1} \d{r} \int_{0}^{2\pi} \d{\varphi} r^{3} \cos(\varphi) \sin(\varphi) \\ | |||||
| &= \frac{1}{4\pi} \int_{0}^{2\pi} \cos(\varphi) \sin(\varphi)\d{\varphi} \\ | |||||
| &\stackrel{\text{(\ref{eq:1})}}{=} 0 | |||||
| \intertext{Da $\E(X) = \E(Y) = 0$ folgt also} | |||||
| \cov(X,Y) &= 0 | |||||
| \intertext{Und damit} | |||||
| \rho(X,Y) &= 0 | |||||
| .\end{salign*} | |||||
| \item Es gilt nach VL: $X \indep Y \iff f^{X,Y}(x,y) = f^{X}(x) f^{Y}(y)$ $\mathscr{L}$-f.ü. Nun | |||||
| betrachte $A \coloneqq (-1,1)^2 \setminus E$. Dann ist | |||||
| \[ | |||||
| \mathscr{L}^2(A) = \mathscr{L}^2(A) - \mathscr{L}^2(E) = 2^2 - \pi = 4 - \pi > 0 | |||||
| .\] Also ist $A$ keine $\mathscr{L}$-Nullmenge. Jedoch gilt $\forall (x,y) \in A$: | |||||
| \[ | |||||
| f^{X,Y}(x,y) = 0 \neq \frac{4}{\pi^2} \underbrace{\sqrt{1-x^2}}_{> 0} \underbrace{\sqrt{1-y^2} }_{> 0} | |||||
| .\] Also folgt $X$ und $Y$ nicht unabhängig. | |||||
| \end{enumerate} | |||||
| \end{aufgabe} | |||||
| \stepcounter{aufgabe} | |||||
| \begin{aufgabe} | |||||
| \begin{enumerate}[(a)] | |||||
| \item Rechnen ergibt für $z \in \R$ | |||||
| \begin{salign*} | |||||
| \mathbb{F}^{M_1}(z) &= \mathbb{P}\left( \{M_1 \le z\} \right) \\ | |||||
| &= \mathbb{P}\left( \left\{ \min_{i \in \{1, \ldots, n\} }{X_i} \le z\right\} \right) \\ | |||||
| &= 1 - \mathbb{P}\left( \bigcap_{i=1}^{n} \{X_i > z\} \right) \\ | |||||
| &\stackrel{\text{unabh.}}{=} | |||||
| 1 - \prod_{i=1}^{n} \mathbb{P}(\{X_i > z\}) \\ | |||||
| &\stackrel{\text{idv}}{=} 1 - (1 - \mathbb{F}^{X}(z))^{n} \\ | |||||
| \mathbb{F}^{M_2}(z) &= \mathbb{P}\left( \{M_2 \le z\} \right) \\ | |||||
| &= \mathbb{P}\left( \prod_{i=1}^{n} \{X_i \le z\} \right) \\ | |||||
| &\stackrel{\text{unabh.}}{=} \prod_{i=1}^{n} \mathbb{P}(\{X_i \le z\}) \\ | |||||
| &\stackrel{\text{idv}}{=} \mathbb{F}^{X}(z)^{n} | |||||
| .\end{salign*} | |||||
| \item Für $X_1 \sim \text{Exp}_{\lambda}$ ist $\mathbb{F}^{X_1} = (1 - \exp(- \lambda z))\mathbbm{1}_{\R^{+}}$. Damit folgt | |||||
| \begin{salign*} | |||||
| \mathbb{F}^{M_1}(z) &= 1 - (1 - \mathbb{F}_{\text{Exp}_{\lambda}}(z))^{n} \\ | |||||
| &= 1 - \left[ 1 - \left( 1 - \exp(-\lambda z) \right) \mathbbm{1}_{\R^{+}(z)} \right]^{n} \\ | |||||
| &= 1 - \left[ 1 - \mathbbm{1}_{\R^{+}}(z) + \exp(- \lambda z) \mathbbm{1}_{\R^{+}}(z)\right]^{n}\\ | |||||
| &= 1 - \begin{cases} | |||||
| \exp(- \lambda n z) & z \in \R^{+} \\ | |||||
| 1 & z \not\in \R^{+} | |||||
| \end{cases}\\ | |||||
| &= (1 - \exp(- \lambda n z)) \mathbbm{1}_{\R^{+}} \\ | |||||
| &= \mathbb{F}_{\text{Exp}_{n\lambda}} | |||||
| .\end{salign*} | |||||
| Da die Verteilungsfunktion das W-Maß eindeutig festlegt, folgt | |||||
| $M_1 \sim \text{Exp}_{n\lambda}$. | |||||
| \item Für $X_1 \sim U_{[0, \theta]}$ ist die Dichte $f(x) = \frac{1}{\theta} \mathbbm{1}_{[0, \theta]}$ | |||||
| gegeben. Damit folgt | |||||
| \begin{salign*} | |||||
| \E_{\theta}(X_1) &= \int_{\R}^{} \frac{x}{\theta} \mathbbm{1}_{[0, \theta]} \d{x} \\ | |||||
| &= \frac{1}{\theta} \int_{0}^{\theta} x \d{x} \\ | |||||
| &= \frac{\theta}{2} \\ | |||||
| \E_{\theta}(X_1^2) &= \int_{\R}^{} \frac{x^2}{\theta} \mathbbm{1}_{[0, \theta]} \d{x} \\ | |||||
| &= \frac{1}{\theta} \int_{0}^{\theta} x^2 \d{x} \\ | |||||
| &= \frac{\theta^2}{3} \\ | |||||
| \var_{\theta}(X_1) &= \E_{\theta}(X_1^2) - \E_{\theta}(X_1)^2 \\ | |||||
| &= \frac{\theta^2}{3} - \frac{\theta^2}{4} \\ | |||||
| &= \frac{\theta^2}{12} | |||||
| .\end{salign*} | |||||
| Es gilt $f^{M_{2}} = (\mathbb{F}^{M_{2}})'$. Damit folgt für $z \in \R$: | |||||
| \begin{salign*} | |||||
| f^{M_2}(z) &= (\mathbb{F}^{M_2})'(z) \\ | |||||
| &= (\mathbb{F}^{X}(z)^{n})' \\ | |||||
| &= n (\mathbb{F}^{X}(z)^{n-1}) f^{X}(z) \\ | |||||
| &= n \left( \frac{(z \land \theta) \lor \theta}{\theta} \right)^{n-1} | |||||
| \frac{1}{\theta} \mathbbm{1}_{[0, \theta]}(z) \\ | |||||
| &= \frac{n}{\theta^{n}} z^{n-1} \mathbbm{1}_{[0, \theta]}(z) | |||||
| \intertext{Damit folgt} | |||||
| \E_{\theta}(M_2) &= \int_{\R}^{} x \frac{n x^{n-1}}{\theta ^{n}} \mathbbm{1}_{[0, \theta]} | |||||
| \d{x} \\ | |||||
| &= \frac{n}{\theta^{n}} \int_{0}^{\theta} x^{n} \d{x} \\ | |||||
| &= \frac{n}{n+1} \theta | |||||
| .\end{salign*} | |||||
| \item Rechnen ergibt | |||||
| \begin{salign*} | |||||
| \E_{\theta}(\overline{X}_n) &= \E_{\theta}\left( \frac{1}{n} \sum_{k=1}^{n} X_k \right) \\ | |||||
| &\stackrel{\text{lin.}}{=} \frac{1}{n} \sum_{k=1}^{n} \E_{\theta}(X_k) \\ | |||||
| &\stackrel{\text{idv}}{=} \E_{\theta}(X_1) \\ | |||||
| &= \frac{\theta}{2} | |||||
| \intertext{Damit folgt} | |||||
| \text{Bias}_{\theta}(\hat{\theta}_1) &= \E_{\theta}(\hat{\theta}_1 - \theta) \\ | |||||
| &= 2 \E_{\theta}(\overline{X}_n) - \theta \\ | |||||
| &= 2 \frac{\theta}{2} - \theta \\ | |||||
| &= 0 \\ | |||||
| \text{Bias}_{\theta}(\hat{\theta}_2) | |||||
| &= \E_{\theta}(\hat{\theta}_2 - \theta) \\ | |||||
| &= \E_{\theta}(M_2) - \theta \\ | |||||
| &= \frac{n}{n+1} \theta - \theta \\ | |||||
| &= - \frac{\theta}{n+1} | |||||
| \intertext{Nun rechne} | |||||
| \E_{\theta}(M_2^2) &= \int_{\R}^{} x^2 \frac{n x^{n-1}}{\theta^{n}} \mathbbm{1}_{[0, \theta]}(x) \d{x} \\ | |||||
| &= \frac{n}{\theta ^{n}} \int_{0}^{\theta} x^{n+1} \d{x} \\ | |||||
| &= \frac{n}{n+2} \theta^2 \tageq \label{eq:2} | |||||
| \intertext{ | |||||
| Es ist offensichtlich $\hat{\theta}_3$ nun erwartungstreu. Damit folgt für $n > 1$} | |||||
| \var_{\theta}(\hat{\theta}_1) &= 4 \var_{\theta}(\overline{X}_n) \\ | |||||
| &\stackrel{\text{unabh.}}{=} \frac{4}{n^2} \sum_{k=1}^{n} \var_{\theta}(X_k) \\ | |||||
| &\stackrel{\text{idv}}{=} \frac{4}{n} \var_{\theta}(X_1) \\ | |||||
| &= \frac{\theta^2}{3n} \\ | |||||
| &> \frac{\theta^2}{n(n+2)} \\ | |||||
| &= \left( \frac{n+1}{n} \right)^2 \frac{n}{n+2} \theta^2 - \theta^2 \\ | |||||
| &\stackrel{\text{(\ref{eq:2})}}{=} \left( \frac{n+1}{n} \right)^2 \E_{\theta}(M_2^2) - \E_{\theta}\left( \frac{n+1}{n} M_2 \right)^2 \\ | |||||
| &= \E_{\theta} (\hat{\theta}_3^2) - \E_{\theta}(\hat{\theta}_3)^2 \\ | |||||
| &= \var_{\theta}(\hat{\theta}_3) | |||||
| \intertext{Schlussendlich ergibt sich} | |||||
| \text{MSE}_{\theta}(\hat{\theta}_1) &= \E_{\theta}(|\hat{\theta}_1 - \theta|^2) \\ | |||||
| &= 4 \E_{\theta}(\overline{X}_n^2) - \theta^2 \\ | |||||
| &= 4 \var_{\theta}(\overline{X}_n) + 4 \E_{\theta}(\overline{X}_n)^2 - \theta^2 \\ | |||||
| &\stackrel{\text{iid}}{=} \frac{4}{n} \var_{\theta}(X_1) \\ | |||||
| &= \frac{\theta^2}{3n} \\ | |||||
| \text{MSE}_{\theta}(\hat{\theta}_2) &= \E_{\theta}(\hat{\theta}_2^2) - 2 \theta \E_{\theta}(M_2) | |||||
| + \theta^2 \\ | |||||
| &= \frac{n}{n+2} \theta^2 - 2 \frac{n}{n+1} \theta^2 | |||||
| + \theta^2 \\ | |||||
| &= \frac{2 \theta^2}{(n+2)(n+1)} \\ | |||||
| \text{MSE}_{\theta}(\hat{\theta}_3) &= \E_{\theta}(\hat{\theta}_3^2) - 2 \theta \E_{\theta} | |||||
| (\hat{\theta}_3) + \theta^2 \\ | |||||
| &= \left( \frac{n+1}{n} \right)^2 \frac{n}{n+2} \theta^2 - \theta^2 \\ | |||||
| &= \frac{\theta^2}{n(n+2)} | |||||
| .\end{salign*} | |||||
| \end{enumerate} | |||||
| \end{aufgabe} | |||||
| \end{document} | |||||