equation 104.29 eq:ewh-vacuum

open in the book · parts/11-qft-standard-model/06-electroweak-higgs.tex:1083

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equation 104.29: eq:ewh-vacuum104.29phenomenon 108.73: Neutrino mass points above the electroweak scale108.73theorem 104.38: Masses, mixing, and where the CKM matrix comes from104.38theorem 104.28: The gauge boson masses104.28equation 104.28: eq:ewh-full-lagrangian104.28equation 108.68: eq:rg-weinberg-operator108.68proof : ch:10-renormalization-group@proof-31proofequation 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-20proofnotation 104.1: Dimensionless couplings and the electroweak scale104.1theorem 104.22: Kibble: the gauge-boson mass matrix104.22theorem 104.41: Ross–Veltman: ρ counts the representation104.41proof : ch:06-electroweak-higgs@proof-13proof

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depends_on Neutrino mass points above the electroweak scale declared parts/11-qft-standard-model/10-renormalization-group.tex:2768
depends_on Masses, mixing, and where the CKM matrix comes from declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1674
depends_on The gauge boson masses declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1224