theorem 104.41 Ross–Veltman: $\rho$ counts the representation

open in the book · parts/11-qft-standard-model/06-electroweak-higgs.tex:1862 · p. 2091

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theorem 104.41: Ross–Veltman: ρ counts the representation104.41equation 104.45: eq:ewh-rho104.45theorem 104.28: The gauge boson masses104.28phenomenon 113.6: The weak bosons are massive and the photon is not113.6proof : ch:06-electroweak-higgs@proof-22prooftheorem 104.40: Custodial symmetry104.40equation 104.29: eq:ewh-vacuum104.29notation 104.1: Dimensionless couplings and the electroweak scale104.1theorem 104.22: Kibble: the gauge-boson mass matrix104.22proof : ch:06-electroweak-higgs@proof-13proofequation 104.36: eq:ewh-masses104.36proposition 104.43: The top contribution to ρ104.43phenomenon 113.17: A new boson near 125 GeV113.17proof : ch:15-exp-higgs-discovery@proof-3proof

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typedirectionnode provenancewhere
cites Neutral currents and the Higgs mechanism derived parts/11-qft-standard-model/06-electroweak-higgs.tex:1879
cites Isospin breaking in technicolor models derived parts/11-qft-standard-model/06-electroweak-higgs.tex:1879
depends_on eq:ewh-rho declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1880
depends_on The gauge boson masses declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1880
depends_on The weak bosons are massive and the photon is not declared parts/11-qft-standard-model/15-exp-higgs-discovery.tex:360
proves ch:06-electroweak-higgs@proof-22 declared parts/11-qft-standard-model/06-electroweak-higgs.tex:1883