theorem 102.25 Gauge fixing needs a determinant

open in the book · parts/11-qft-standard-model/04-qcd.tex:972 · p. 2000

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theorem 102.25: Gauge fixing needs a determinant102.25corollary 106.53: Why electrodynamics has no ghosts106.53equation 102.23: eq:qcd-gauge-infinitesimal102.23theorem 106.52: Faddeev–Popov106.52proposition 102.29: Feynman rules for QCD in SI form102.29theorem 102.26: Non-abelian gauge theories are renormalizable102.26proof : ch:04-qcd@proof-11proofequation 106.69: eq:pathint-fp-operator106.69equation 100.16: eq:qed-gauge-fixing-term100.16equation 106.67: eq:pathint-gauge-transformation106.67proposition 106.51: The naive integral diverges by the volume of the gauge group106.51proof : ch:08-path-integral-quantization@proof-37proofequation 102.28: eq:qcd-ym-expanded102.28proposition 100.14: The Feynman rules of QED in SI form100.14proof : ch:04-qcd@proof-13prooftheorem 100.17: Superficial degree of divergence100.17pending : ch:04-qcd@pending-1pendingproposition 102.28: The parameters of QCD102.28

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typedirectionnode provenancewhere
cites Feynman diagrams for the Yang-Mills field derived parts/11-qft-standard-model/04-qcd.tex:978
depends_on Why electrodynamics has no ghosts declared parts/11-qft-standard-model/04-qcd.tex:985
depends_on eq:qcd-gauge-infinitesimal declared parts/11-qft-standard-model/04-qcd.tex:985
depends_on Faddeev–Popov declared parts/11-qft-standard-model/04-qcd.tex:985
depends_on Feynman rules for QCD in SI form declared parts/11-qft-standard-model/04-qcd.tex:1175
depends_on Non-abelian gauge theories are renormalizable declared parts/11-qft-standard-model/04-qcd.tex:1043
proves ch:04-qcd@proof-11 declared parts/11-qft-standard-model/04-qcd.tex:989