equation 104.46 eq:ewh-yukawa-lagrangian

open in the book · parts/11-qft-standard-model/06-electroweak-higgs.tex:1611

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equation 104.46: eq:ewh-yukawa-lagrangian104.46proposition 104.61: The couplings are the masses divided by v104.61proposition 104.42: The sources of custodial violation104.42theorem 105.25: Number of physical phases105.25theorem 104.38: Masses, mixing, and where the CKM matrix comes from104.38equation 104.34: eq:ewh-gauge-mass-terms104.34experiment : The Higgs Boson Discoveryexperime…phenomenon 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-34prooftheorem 104.40: Custodial symmetry104.40proposition 104.43: The top contribution to ρ104.43proof : ch:06-electroweak-higgs@proof-23proofproposition 105.27: When CP violation is possible105.27proof : ch:07-discrete-symmetries-cpt@proof-20proofequation 104.29: eq:ewh-vacuum104.29theorem 101.59: Glashow–Iliopoulos–Maiani101.59phenomenon 104.59: A neutral scalar boson exists104.59phenomenon 103.10: There are no flavour-changing neutral currents103.10proof : ch:06-electroweak-higgs@proof-20proof

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typedirectionnode provenancewhere
depends_on The couplings are the masses divided by $v$ declared parts/11-qft-standard-model/06-electroweak-higgs.tex:3188
depends_on The sources of custodial violation declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1940
depends_on Number of physical phases declared parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2079
depends_on Masses, mixing, and where the CKM matrix comes from declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1674