theorem 107.29 Chiral power counting for the nuclear force

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theorem 107.29: Chiral power counting for the nuclear force107.29proposition 102.67: The chiral symmetry of massless quarks102.67theorem 102.70: Goldstone102.70equation 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 doublets102.68proof : ch:04-qcd@proof-34proofequation 102.75: eq:qcd-breaking-pattern102.75phenomenon 102.72: The pion is anomalously light102.72proof : ch:04-qcd@proof-36proof

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cites Nuclear forces from chiral lagrangians derived parts/11-qft-standard-model/09-nuclear-physics.tex:1244
depends_on The chiral symmetry of massless quarks declared parts/11-qft-standard-model/09-nuclear-physics.tex:1248
depends_on Goldstone declared parts/11-qft-standard-model/09-nuclear-physics.tex:1248