proposition 102.67 The chiral symmetry of massless quarks

open in the book · parts/11-qft-standard-model/04-qcd.tex:2796 · p. 2021

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proposition 102.67: The chiral symmetry of massless quarks102.67equation 102.21: eq:qcd-covariant-derivative102.21equation 102.29: eq:qcd-lagrangian102.29theorem 106.87: The axial anomaly106.87phenomenon 102.68: The spectrum has no parity doublets102.68theorem 107.29: Chiral power counting for the nuclear force107.29proof : ch:04-qcd@proof-34proofphenomenon 102.64: Almost none of the proton's mass comes from quark masses102.64phenomenon 102.39: A mass scale from a dimensionless coupling102.39proposition 102.28: The parameters of QCD102.28proposition 102.76: QCD permits one more term102.76equation 106.99: eq:pathint-chiral-rotation106.99proposition 106.85: Classical conservation of the axial current106.85proposition 102.16: The neutral pion width counts colours squared102.16equation 102.74: eq:qcd-chiral-group102.74phenomenon 102.72: The pion is anomalously light102.72theorem 102.70: Goldstone102.70proof : ch:04-qcd@proof-35proof

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typedirectionnode provenancewhere
depends_on eq:qcd-covariant-derivative declared parts/11-qft-standard-model/04-qcd.tex:2816
depends_on eq:qcd-lagrangian declared parts/11-qft-standard-model/04-qcd.tex:2816
depends_on The axial anomaly declared parts/11-qft-standard-model/04-qcd.tex:2816
depends_on The spectrum has no parity doublets declared parts/11-qft-standard-model/04-qcd.tex:2860
depends_on Chiral power counting for the nuclear force declared parts/11-qft-standard-model/09-nuclear-physics.tex:1248
proves ch:04-qcd@proof-34 declared parts/11-qft-standard-model/04-qcd.tex:2820