phenomenon 103.10 There are no flavour-changing neutral currents

open in the book · parts/11-qft-standard-model/05-flavour-neutrinos.tex:382 · p. 2033

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phenomenon 103.10: There are no flavour-changing neutral currents103.10theorem 104.38: Masses, mixing, and where the CKM matrix comes from104.38theorem 101.59: Glashow–Iliopoulos–Maiani101.59proof : ch:05-flavour-neutrinos@proof-5proofequation 104.29: eq:ewh-vacuum104.29equation 104.46: eq:ewh-yukawa-lagrangian104.46phenomenon 104.59: A neutral scalar boson exists104.59proposition 104.61: The couplings are the masses divided by v104.61proof : ch:06-electroweak-higgs@proof-20proofequation 101.62: eq:weak-cabibbo-rotation101.62proposition 101.58: A single rotated doublet produces a flavour-changing neutral current101.58proposition 101.63: Parameter counting, and why three generations permit CP violation101.63proof : ch:03-weak-interactions@proof-42proof

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typedirectionnode provenancewhere
cites Review of Particle Physics derived parts/11-qft-standard-model/05-flavour-neutrinos.tex:388
depends_on Masses, mixing, and where the CKM matrix comes from declared parts/11-qft-standard-model/05-flavour-neutrinos.tex:394
depends_on Glashow–Iliopoulos–Maiani declared parts/11-qft-standard-model/05-flavour-neutrinos.tex:394
proves ch:05-flavour-neutrinos@proof-5 declared parts/11-qft-standard-model/05-flavour-neutrinos.tex:397