"Constrained system : U(1) pure gauge theory"의 두 판 사이의 차이
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+ | U(1) pure gauge theory : theory of light (without matter) | ||
+ | <math>\mathcal{L}_{\text{free}} = - \frac{1}{4}F_{\mu\nu}F^{\mu\nu}</math> | ||
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+ | quantization of the photon field | ||
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+ | [http://www.ecm.ub.es/%7Eespriu/teaching/classes/fae/LECT4.pdf http://www.ecm.ub.es/~espriu/teaching/classes/fae/LECT4.pdf] | ||
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+ | gives physical and unphysical states | ||
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+ | Hilbert space of physical states | ||
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+ | quantize unconstrained system and then impose the constraint | ||
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+ | remark | ||
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+ | if matter exists, we get [[QED]] | ||
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+ | <math>\mathcal{L}_{\text{free}} = \bar{\psi} (i\gamma^\mu \partial_\mu -m)\psi - \frac{1}{4}F_{\mu\nu}F^{\mu\nu}</math> |
2011년 9월 20일 (화) 07:02 판
U(1) pure gauge theory : theory of light (without matter)
\(\mathcal{L}_{\text{free}} = - \frac{1}{4}F_{\mu\nu}F^{\mu\nu}\)
quantization of the photon field
http://www.ecm.ub.es/~espriu/teaching/classes/fae/LECT4.pdf
gives physical and unphysical states
Hilbert space of physical states
quantize unconstrained system and then impose the constraint
remark
if matter exists, we get QED
\(\mathcal{L}_{\text{free}} = \bar{\psi} (i\gamma^\mu \partial_\mu -m)\psi - \frac{1}{4}F_{\mu\nu}F^{\mu\nu}\)