proposition 101.68 The low-energy limit reproduces Fermi

open in the book · parts/11-qft-standard-model/03-weak-interactions.tex:3246 · p. 1978

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proposition 101.68: The low-energy limit reproduces Fermi101.68equation 100.17: eq:qed-photon-propagator100.17equation 101.46: eq:weak-muon-lagrangian101.46proposition 100.14: The Feynman rules of QED in SI form100.14proposition 101.70: The effective neutral-current interaction101.70proof : ch:03-weak-interactions@proof-47prooftheorem 100.25: One-photon exchange is the Coulomb potential100.25theorem 100.17: Superficial degree of divergence100.17phenomenon 101.53: Charged-current lepton flavour is conserved101.53theorem 101.48: The muon decay rate101.48equation 100.2: eq:qed-action100.2proposition 100.8: The photon propagator100.8theorem 100.5: The gauge principle100.5lemma 100.22: Spin sums100.22proposition 102.29: Feynman rules for QCD in SI form102.29proposition 100.24: Cross-section master formula100.24proposition 101.45: Decay-rate master formula101.45theorem 100.41: Schwinger100.41theorem 100.35: One-loop electron self-energy100.35theorem 100.31: One-loop vacuum polarization100.31proof : ch:02-qed-renormalization@proof-7proofequation 101.75: eq:weak-gv-ga101.75equation 101.74: eq:weak-z-coupling101.74phenomenon 101.72: Neutrinos scatter without becoming charged leptons101.72proof : ch:03-weak-interactions@proof-48proof

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typedirectionnode provenancewhere
depends_on eq:qed-photon-propagator declared parts/11-qft-standard-model/03-weak-interactions.tex:3275
depends_on eq:weak-muon-lagrangian declared parts/11-qft-standard-model/03-weak-interactions.tex:3275
depends_on The Feynman rules of QED in SI form declared parts/11-qft-standard-model/03-weak-interactions.tex:3275
depends_on The effective neutral-current interaction declared parts/11-qft-standard-model/03-weak-interactions.tex:3368
proves ch:03-weak-interactions@proof-47 declared parts/11-qft-standard-model/03-weak-interactions.tex:3279