From f144be56b0c7ec03f74c46928b1354a959a59246 Mon Sep 17 00:00:00 2001 From: =?UTF-8?q?Andreas=20M=C3=BCller?= Date: Sun, 22 May 2022 13:36:59 +0200 Subject: add hermite application presentation --- vorlesungen/slides/hermite/normalhermite.tex | 88 ++++++++++++++++++++++++++++ 1 file changed, 88 insertions(+) create mode 100644 vorlesungen/slides/hermite/normalhermite.tex (limited to 'vorlesungen/slides/hermite/normalhermite.tex') diff --git a/vorlesungen/slides/hermite/normalhermite.tex b/vorlesungen/slides/hermite/normalhermite.tex new file mode 100644 index 0000000..bcd30f2 --- /dev/null +++ b/vorlesungen/slides/hermite/normalhermite.tex @@ -0,0 +1,88 @@ +% +% normalhermite.tex -- integrability of hermite polynomials +% +% (c) 2021 Prof Dr Andreas Müller, OST Ostschweizer Fachhochschule +% +\bgroup +\begin{frame}[t] +\setlength{\abovedisplayskip}{5pt} +\setlength{\belowdisplayskip}{5pt} +\frametitle{Hermite-Polynome} +\vspace{-20pt} +\begin{columns}[t,onlytextwidth] +\begin{column}{0.48\textwidth} +\begin{block}{Definition (Rodrigues-Formel)} +\[ +H_n(x) += +(-1)^n e^{x^2} \frac{d^n}{dx^n} e^{-x^2} +\] +\end{block} +\vspace{-10pt} +\begin{block}{Orthogonalität} +$H_n(x)$ sind orthogonale Polynome bezüglich $w(x)=e^{-x^2}$, d.~h. +\begin{align*} +\langle H_n,H_m\rangle_w +&= +\int H_n(x)H_m(x)e^{-x^2}\,dx +\\ +&= +\biggl\{ +\renewcommand{\arraycolsep}{1pt} +\begin{array}{l@{\quad}l} +1&\text{falls $n=m$}\\ +0&\text{sonst} +\end{array} +\biggr\} += +\delta_{mn} +\end{align*} +\end{block} +\vspace{-10pt} +\begin{block}{Rekursion: Auf-/Absteigeoperatoren} +Rekursionsformel: +\[ +H_n(x) += +2x\cdot H_{n-1}(x) - H_{n-1}'(x) +\] +\end{block} +\end{column} +\begin{column}{0.48\textwidth} +\begin{block}{Stammfunktion} +\begin{align*} +\int H_n(x) e^{-x^2}\,dx +&= +\int \bigl({\color{red}2x}H_{n-1}(x) +\\ +&\qquad -H_{n-1}'(x)\bigr) e^{-x^2}\,dx +\\ +{\color{gray}(e^{-x^2}=-2x)} +&= +{\color{red}-}\int {\color{red}(e^{-x^2})'} H_{n-1}(x)\,dx +\\ +&\qquad +- +\int H_{n-1}'(x) e^{-x^2}\,dx +\\ +\text{\color{gray}(Produktregel)} +&= +\int (e^{-x^2}H_{n-1}(x))'\,dx +\\ +\text{\color{gray}(Ableitung)} +&= +e^{-x^2}H_{n-1}(x) +\end{align*} +ausser für $n=0$: +\[ +\int +H_0(x)e^{-x^2}\,dx += +\int +e^{-x^2}\,dx +\] +\end{block} +\end{column} +\end{columns} +\end{frame} +\egroup -- cgit v1.2.1 From 1b887f44b5ec310f00184c916623d59abcf6e14d Mon Sep 17 00:00:00 2001 From: =?UTF-8?q?Andreas=20M=C3=BCller?= Date: Sun, 22 May 2022 15:21:28 +0200 Subject: typo --- vorlesungen/slides/hermite/normalhermite.tex | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) (limited to 'vorlesungen/slides/hermite/normalhermite.tex') diff --git a/vorlesungen/slides/hermite/normalhermite.tex b/vorlesungen/slides/hermite/normalhermite.tex index bcd30f2..16a314c 100644 --- a/vorlesungen/slides/hermite/normalhermite.tex +++ b/vorlesungen/slides/hermite/normalhermite.tex @@ -57,7 +57,7 @@ H_n(x) \\ &\qquad -H_{n-1}'(x)\bigr) e^{-x^2}\,dx \\ -{\color{gray}(e^{-x^2}=-2x)} +{\color{gray}((e^{-x^2})'=-2x)} &= {\color{red}-}\int {\color{red}(e^{-x^2})'} H_{n-1}(x)\,dx \\ -- cgit v1.2.1 From 83d215597b5df724022de2a08ae1dfa1e8d59497 Mon Sep 17 00:00:00 2001 From: =?UTF-8?q?Andreas=20M=C3=BCller?= Date: Thu, 2 Jun 2022 23:01:38 +0200 Subject: phases --- vorlesungen/slides/hermite/normalhermite.tex | 29 +++++++++++++++++++++------- 1 file changed, 22 insertions(+), 7 deletions(-) (limited to 'vorlesungen/slides/hermite/normalhermite.tex') diff --git a/vorlesungen/slides/hermite/normalhermite.tex b/vorlesungen/slides/hermite/normalhermite.tex index 16a314c..98721dc 100644 --- a/vorlesungen/slides/hermite/normalhermite.tex +++ b/vorlesungen/slides/hermite/normalhermite.tex @@ -19,6 +19,7 @@ H_n(x) \] \end{block} \vspace{-10pt} +\uncover<2->{% \begin{block}{Orthogonalität} $H_n(x)$ sind orthogonale Polynome bezüglich $w(x)=e^{-x^2}$, d.~h. \begin{align*} @@ -37,8 +38,9 @@ $H_n(x)$ sind orthogonale Polynome bezüglich $w(x)=e^{-x^2}$, d.~h. = \delta_{mn} \end{align*} -\end{block} +\end{block}} \vspace{-10pt} +\uncover<3->{% \begin{block}{Rekursion: Auf-/Absteigeoperatoren} Rekursionsformel: \[ @@ -46,33 +48,46 @@ H_n(x) = 2x\cdot H_{n-1}(x) - H_{n-1}'(x) \] -\end{block} +\end{block}} \end{column} \begin{column}{0.48\textwidth} +\uncover<4->{% \begin{block}{Stammfunktion} \begin{align*} -\int H_n(x) e^{-x^2}\,dx -&= -\int \bigl({\color{red}2x}H_{n-1}(x) +\uncover<4->{ +\int H_n(x) e^{-x^2}\,dx} +&\uncover<5->{= +\int \bigl({\color{red}2x}H_{n-1}(x)} \\ +\uncover<5->{ &\qquad -H_{n-1}'(x)\bigr) e^{-x^2}\,dx +} \\ +\uncover<6->{ {\color{gray}((e^{-x^2})'=-2x)} &= {\color{red}-}\int {\color{red}(e^{-x^2})'} H_{n-1}(x)\,dx +} \\ +\uncover<6->{ &\qquad - \int H_{n-1}'(x) e^{-x^2}\,dx +} \\ +\uncover<7->{ \text{\color{gray}(Produktregel)} &= \int (e^{-x^2}H_{n-1}(x))'\,dx +} \\ +\uncover<8->{ \text{\color{gray}(Ableitung)} &= e^{-x^2}H_{n-1}(x) +} \end{align*} +\uncover<9->{% ausser für $n=0$: \[ \int @@ -80,8 +95,8 @@ H_0(x)e^{-x^2}\,dx = \int e^{-x^2}\,dx -\] -\end{block} +\]} +\end{block}} \end{column} \end{columns} \end{frame} -- cgit v1.2.1