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Haifeng Yang edited Quantize K-G Field.tex
over 10 years ago
Commit id: 8470006100a323455dbb1bc666c01ee33d876328
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diff --git a/Quantize K-G Field.tex b/Quantize K-G Field.tex
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\subsection{Quantize Klein-Gordon}
Fourier Transformation: \subsubsection{Fourier Transformation}
$$\hat{\phi}(\mathbf{x}) = \int \frac{d^3 k}{(2\pi)^3 } \hat{\tilde{\phi}}(\mathbf{k})e^{i\mathbf{k}\cdot \mathbf{x}}$$
$$\hat{\pi}(\mathbf{y}) = \int \frac{d^3 k}{(2\pi)^3 } \hat{\tilde{\pi}}(\mathbf{k})e^{i\mathbf{k}\cdot \mathbf{y}}$$
...
+\frac{1}{2}\omega_\mathbf{k}^2 \hat{\tilde{\phi}}(\mathbf{k})^\dagger \hat{\tilde{\phi}}(\mathbf{k})
\right]$$
Note: These are complex harmonic oscillators.
$\tilde{\phi}(-\mathbf{k})=\tilde{\phi}(\mathbf{k})^*$ $\tilde{\phi}(-\mathbf{k})=\tilde{\phi}(\mathbf{k})^*$. All $\mathbf{k}$'s are not independent.
\subsubsection{Commutation Relations}
$$[\hat{\tiled{\pi}}(\mathbf{k'}), \hat{\tilde{\phi}}(\mathbf{k})] = - i (2\pi)^3 \delta^{(3)} (\mathbf{k} + \mathbf{k'})$$