phenomenon 101.40 The vector coupling is not renormalized

open in the book · parts/11-qft-standard-model/03-weak-interactions.tex:1889 · p. 1963

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phenomenon 101.40: The vector coupling is not renormalized101.40phenomenon 101.18: Superallowed decays measure one number101.18proposition 100.6: The coupling is universal100.6phenomenon 101.43: One coupling governs every charged-current process101.43proof : ch:03-weak-interactions@proof-27proofequation 101.17: eq:weak-ft101.17proposition 101.15: Allowed selection rules101.15proof : ch:03-weak-interactions@proof-13proofequation 100.9: eq:qed-covariant-derivative100.9equation 100.7: eq:qed-local-phase100.7theorem 100.5: The gauge principle100.5proof : ch:02-qed-renormalization@proof-2proofequation 101.20: eq:weak-Ft-formula101.20equation 101.53: eq:weak-muon-rate101.53phenomenon 103.7: Strangeness-changing decays are suppressed, by one angle103.7phenomenon 101.55: Strangeness-changing decays are suppressed by one angle101.55proof : ch:03-weak-interactions@proof-29proof

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typedirectionnode provenancewhere
cites Review of Particle Physics derived parts/11-qft-standard-model/03-weak-interactions.tex:1897
depends_on Superallowed decays measure one number declared parts/11-qft-standard-model/03-weak-interactions.tex:1898
depends_on The coupling is universal declared parts/11-qft-standard-model/03-weak-interactions.tex:1898
depends_on One coupling governs every charged-current process declared parts/11-qft-standard-model/03-weak-interactions.tex:2080
proves ch:03-weak-interactions@proof-27 declared parts/11-qft-standard-model/03-weak-interactions.tex:1901