theorem 104.38 Masses, mixing, and where the CKM matrix comes from

open in the book · parts/11-qft-standard-model/06-electroweak-higgs.tex:1653 · p. 2089

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theorem 104.38: Masses, mixing, and where the CKM matrix comes from104.38equation 104.29: eq:ewh-vacuum104.29equation 104.46: eq:ewh-yukawa-lagrangian104.46theorem 101.59: Glashow–Iliopoulos–Maiani101.59phenomenon 104.59: A neutral scalar boson exists104.59phenomenon 103.10: There are no flavour-changing neutral currents103.10proposition 104.61: The couplings are the masses divided by v104.61proof : ch:06-electroweak-higgs@proof-20proofphenomenon 108.73: Neutrino mass points above the electroweak scale108.73theorem 104.28: The gauge boson masses104.28proposition 104.42: The sources of custodial violation104.42theorem 105.25: Number of physical phases105.25equation 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-42proofequation 101.86: eq:weak-z-width101.86table 104.2: tab:ewh-yukawa104.2proof : ch:06-electroweak-higgs@proof-32proofexperiment : The Higgs Boson Discoveryexperime…proof : ch:05-flavour-neutrinos@proof-5proofequation 104.34: eq:ewh-gauge-mass-terms104.34phenomenon 104.62: The scalar couples in proportion to mass104.62phenomenon 113.24: Couplings proportional to mass113.24proposition 113.5: One number is unknown, and it is the mass113.5proof : ch:06-electroweak-higgs@proof-34proof

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typedirectionnode provenancewhere
depends_on eq:ewh-vacuum declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1674
depends_on eq:ewh-yukawa-lagrangian declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1674
depends_on Glashow–Iliopoulos–Maiani declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1674
depends_on A neutral scalar boson exists declared parts/11-qft-standard-model/06-electroweak-higgs.tex:3001
depends_on There are no flavour-changing neutral currents declared parts/11-qft-standard-model/05-flavour-neutrinos.tex:394
depends_on The couplings are the masses divided by $v$ declared parts/11-qft-standard-model/06-electroweak-higgs.tex:3188
proves ch:06-electroweak-higgs@proof-20 declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1677