From a1b5390cd72b552fdc759f4892f802c52cf9a4ff Mon Sep 17 00:00:00 2001 From: =?UTF-8?q?Oliver=20Gro=C3=9F?= Date: Fri, 8 Aug 2008 14:28:22 +0200 Subject: [PATCH] Kapitel III.1 fertig --- kapIII-1.tex | 40 ++++++++++++++++++++++++++++++++++++++++ 1 file changed, 40 insertions(+) create mode 100644 kapIII-1.tex diff --git a/kapIII-1.tex b/kapIII-1.tex new file mode 100644 index 0000000..d9d6688 --- /dev/null +++ b/kapIII-1.tex @@ -0,0 +1,40 @@ +\begin{landscape} + \chapter{Übersicht und Notation} + \begin{tabular}{l||l|l|l} + & $d = 1$ & $d = 2$ & $d = 3$ \\ \hline \hline + SG: $i\hbar \ket{\psi} = H \ket{\psi}$ & + $\checkmark$ & + $\checkmark$ & + $\checkmark$ \\ \hline + Hamiltonoperator: $H$ & + $\frac{\hat{p}^2}{2m} + V(\hat{x})$ & + $\frac{\hat{p}_x^2}{2m} + \frac{\hat{p}_y^2}{2m} + V(\hat{x}, \hat{y})$ & + $\frac{\hat{p}_x^2}{2m} + \frac{\hat{p}_y^2}{2m} + \frac{\hat{p}_z^2}{2m} + V(\hat{x}, \hat{y}, \hat{z})$ \\ \hline + Kommutator & + $[\hat{x}, \hat{y}] = i\hbar$ & + $[\hat{x}_k, \hat{y}_l] = i\hbar \krondelta{k,l};~ k, l = 1, 2$ & + $[\hat{x}_k, \hat{y}_l] = i\hbar \krondelta{k,l};~ k, l = 1, 2, 3$ \\ \hline + stationäre SG: $H \ket{\phi} = E \ket{\psi}$ & + gewöhnliche DGL & + partielle DGL & + partielle DGL\\ \hline + Rotationsinvarianz & + Irrelevant & + $V(x,y) = V(\rho)$; $\rho \equiv \sqrt{x^2 + y^2}$ & + $V(x,y,z) = V(r)$; $r \equiv \sqrt{x^2 + y^2 + z^2}$ \\ \hline + Ortseingen-vektoren & + $\hat{x}\ket{x} = x \ket{x}$ & + $\ket{x,y} \cequiv \ket{\rho, \theta}$ & + $\ket{x,y,z} \cequiv \ket{\rho, \theta, \varphi}$ \\ \hline + Norm der Wellenfunktion & + \begin{math}1 = \intgr{-\infty}{+\infty}{\abs{\psi(x)}^2}{x}\end{math} & + $\begin{array}{l} + 1 = \intgr{-\infty}{+\infty}{\intgr{-\infty}{+\infty}{\abs{\psi(x,y)}^2}{y}}{x} \\ + \hphantom{1} = \intgr{0}{\infty}{\rho \intgr{0}{2\pi}{\abs{\psi(\rho, \varphi)}^2}{\varphi}}{\rho} + \end{array}$ & + $\begin{array}{l} + 1 = \intgru{\intgru{\intgru{\abs{\psi(x,y,z)}^2}{x}}{y}}{z} \\ + \hphantom{1} = \intgr{0}{+\infty}{r^2 \intgr{-1}{+1}{\intgr{0}{2\pi}{\abs{\psi}^2}{\varphi}}{(\cos\theta)}}{r} + \end{array}$ \\ \hline + \end{tabular} +\end{landscape}