theorem 106.87 The axial anomaly

open in the book · parts/11-qft-standard-model/08-path-integral-quantization.tex:4123 · p. 2201

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theorem 106.87: The axial anomaly106.87equation 106.99: eq:pathint-chiral-rotation106.99proposition 106.85: Classical conservation of the axial current106.85proposition 102.67: The chiral symmetry of massless quarks102.67proposition 102.16: The neutral pion width counts colours squared102.16theorem 106.93: Fujikawa106.93equation 100.5: eq:qed-free-dirac100.5proof : ch:08-path-integral-quantization@proof-58proofequation 102.21: eq:qcd-covariant-derivative102.21equation 102.29: eq:qcd-lagrangian102.29phenomenon 102.68: The spectrum has no parity doublets102.68theorem 107.29: Chiral power counting for the nuclear force107.29proof : ch:04-qcd@proof-34proofequation 106.103: eq:pathint-pi0-width106.103theorem 106.89: Adler–Bardeen106.89proof : ch:04-qcd@proof-7proof

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typedirectionnode provenancewhere
depends_on eq:pathint-chiral-rotation declared parts/11-qft-standard-model/08-path-integral-quantization.tex:4137
depends_on Classical conservation of the axial current declared parts/11-qft-standard-model/08-path-integral-quantization.tex:4137
depends_on The chiral symmetry of massless quarks declared parts/11-qft-standard-model/04-qcd.tex:2816
depends_on The neutral pion width counts colours squared declared parts/11-qft-standard-model/04-qcd.tex:660