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Haifeng Yang edited Klein-Gordon Equation.tex
over 10 years ago
Commit id: ed1a61e8a11df8271d5dcb96491fc68c68dfecde
deletions | additions
diff --git a/Klein-Gordon Equation.tex b/Klein-Gordon Equation.tex
index 60fff16..f99add6 100644
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$$\hbar^2 (-\partial_{ct}^2 +\nabla^2) \psi = M^2 c^2 \psi$$
$$-\hbar^2\partial^\mu\partial_\mu \psi = M^2c^2 \psi$$
\begin{enumerate}
\item Problems \subsection{Problems with
K-G. K-G.}
Problem: $|\psi|^2$ is no longer prob. density. Not conserved.
...
Classical limit: $\ddot{\phi} = (c^2\nabla^2 -\frac{(Mc^2)^2}{\hbar^2})\phi \Longrightarrow \ddot{\phi} = (c^2\nabla^2 - \omega_{min}^2)\phi$
\item K-G \subsection{K-G arises in CM
physics physics}
\begin{enumerate}
\item $M=0$ case: $\ddot{\phi} = c^2 \nabla^2 \phi$. Dispersion relation: (Note, $c$ is the wave speed, not speed of light.)
...
\end{enumerate}
\item Quantizing \subsection{Quantizing K-G equation: $\ddot{\phi} = (\nabla^2 -
m^2)\phi$ m^2)\phi$}
\begin{enumerate}
\item Action:
$$S[\phi(\mathbf{x},t)] = \int$$
\end{enumerate}
\end{enumerate}