"Current algebra and anomalies in gauge field theory"의 두 판 사이의 차이

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==internal algebra of symmetry==
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* an internal symmetry is defined by the algebra of generators
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$$
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[I_{\alpha},I_{\beta}]=c_{\alpha \beta \gamma}I_{\gamma}
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$$
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* the generators, in turn, are given by the integral over the time-component of the currents
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$$
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I_{\alpha}=\int d^3x J_{0,\alpha}(x)
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$$
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* from these equations one obtains the equal-time commutation relation of the currents
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$$
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[J_{0,\alpha}(\mathbf{x}),J_{0,\beta}(\mathbf{y})]=c_{\alpha \beta \gamma} J_{0,\alpha}(\mathbf{x})\delta(\mathbf{x}-\mathbf{y})
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$$
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* See [Pietschmann2011] and [[QCD and quarks]] for more
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* [[QCD and quarks]]
 
* [[QCD and quarks]]
 
* [[WZW (Wess-Zumino-Witten) model]]
 
* [[WZW (Wess-Zumino-Witten) model]]
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* http://isites.harvard.edu/fs/docs/icb.topic1146666.files/IV-6-Anomalies.pdf
 
* http://isites.harvard.edu/fs/docs/icb.topic1146666.files/IV-6-Anomalies.pdf
 
* Abel, [http://www.maths.dur.ac.uk/~dma0saa/lecture_notes.pdf Anomalies]
 
* Abel, [http://www.maths.dur.ac.uk/~dma0saa/lecture_notes.pdf Anomalies]
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* [Pietschmann2011] Pietschmann, Herbert. “On the Early History of Current Algebra.” The European Physical Journal H 36, no. 1 (July 2011): 75–84. doi:10.1140/epjh/e2011-20013-0.

2015년 3월 7일 (토) 03:43 판

internal algebra of symmetry

  • an internal symmetry is defined by the algebra of generators

$$ [I_{\alpha},I_{\beta}]=c_{\alpha \beta \gamma}I_{\gamma} $$

  • the generators, in turn, are given by the integral over the time-component of the currents

$$ I_{\alpha}=\int d^3x J_{0,\alpha}(x) $$

  • from these equations one obtains the equal-time commutation relation of the currents

$$ [J_{0,\alpha}(\mathbf{x}),J_{0,\beta}(\mathbf{y})]=c_{\alpha \beta \gamma} J_{0,\alpha}(\mathbf{x})\delta(\mathbf{x}-\mathbf{y}) $$