proposition 102.29 Feynman rules for QCD in SI form

open in the book · parts/11-qft-standard-model/04-qcd.tex:1135 · p. 2001

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proposition 102.29: Feynman rules for QCD in SI form102.29equation 102.28: eq:qcd-ym-expanded102.28proposition 100.14: The Feynman rules of QED in SI form100.14theorem 102.25: Gauge fixing needs a determinant102.25proof : ch:04-qcd@proof-13prooflemma 102.32: Landau levels with g=2102.32equation 100.2: eq:qed-action100.2proposition 100.8: The photon propagator100.8theorem 100.5: The gauge principle100.5lemma 100.22: Spin sums100.22proposition 100.24: Cross-section master formula100.24proposition 101.45: Decay-rate master formula101.45proposition 101.68: The low-energy limit reproduces Fermi101.68theorem 100.25: One-photon exchange is the Coulomb potential100.25theorem 100.41: Schwinger100.41theorem 100.35: One-loop electron self-energy100.35theorem 100.31: One-loop vacuum polarization100.31proof : ch:02-qed-renormalization@proof-7proofcorollary 106.53: Why electrodynamics has no ghosts106.53equation 102.23: eq:qcd-gauge-infinitesimal102.23theorem 106.52: Faddeev–Popov106.52theorem 102.26: Non-abelian gauge theories are renormalizable102.26proof : ch:04-qcd@proof-11proof

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typedirectionnode provenancewhere
depends_on eq:qcd-ym-expanded declared parts/11-qft-standard-model/04-qcd.tex:1175
depends_on The Feynman rules of QED in SI form declared parts/11-qft-standard-model/04-qcd.tex:1175
depends_on Gauge fixing needs a determinant declared parts/11-qft-standard-model/04-qcd.tex:1175
proves ch:04-qcd@proof-13 declared parts/11-qft-standard-model/04-qcd.tex:1179