equation 102.29 eq:qcd-lagrangian

open in the book · parts/11-qft-standard-model/04-qcd.tex:1062

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depends_on phenomenon 102.64 Almost none of the proton's mass comes from quark masses ¶
depends_on phenomenon 102.39 A mass scale from a dimensionless coupling ¶
- depends_on phenomenon 102.64 Almost none of the proton's mass comes from quark masses ¶ ↺
depends_on proposition 102.67 The chiral symmetry of massless quarks ¶
- depends_on phenomenon 102.68 The spectrum has no parity doublets ¶
  - depends_on phenomenon 102.72 The pion is anomalously light ¶
  - depends_on theorem 102.70 Goldstone ¶
    - depends_on phenomenon 102.72 The pion is anomalously light ¶ ↺
    - depends_on theorem 107.29 Chiral power counting for the nuclear force ¶
- depends_on theorem 107.29 Chiral power counting for the nuclear force ¶ ↺
depends_on proposition 102.28 The parameters of QCD ¶
depends_on proposition 102.76 QCD permits one more term ¶
- depends_on phenomenon 102.77 The neutron has no measurable electric dipole moment ¶

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Edges

type	direction	node	provenance	where
`depends_on`	←	Almost none of the proton's mass comes from quark masses	declared	parts/11-qft-standard-model/04-qcd.tex:2675
`depends_on`	←	A mass scale from a dimensionless coupling	declared	parts/11-qft-standard-model/04-qcd.tex:1579
`depends_on`	←	The chiral symmetry of massless quarks	declared	parts/11-qft-standard-model/04-qcd.tex:2816
`depends_on`	←	The parameters of QCD	declared	parts/11-qft-standard-model/04-qcd.tex:1083
`depends_on`	←	QCD permits one more term	declared	parts/11-qft-standard-model/04-qcd.tex:3227