phenomenon 110.19 The weak charge of the proton is small

open in the book · parts/11-qft-standard-model/12-exp-parity-violation.tex:1927 · p. 2352

phenomenon-tested: no experiment declares a \tests edge to it and it is not listed in untested.txt

Rests on

depends_on phenomenon 104.55 One mixing angle describes every neutral-current measurement ¶
- depends_on equation 104.35 eq:ewh-neutral-rotation ¶
- depends_on equation 104.40 eq:ewh-tree-relations ¶
- depends_on proposition 101.67 The mixing angle and the fermion couplings ¶
  - depends_on equation 101.70 eq:weak-covariant-derivative ¶
  - proves proof ch:03-weak-interactions@proof-46 ¶
- proves proof ch:06-electroweak-higgs@proof-29 ¶
depends_on phenomenon 110.17 Parity violation in electron scattering ¶
- depends_on phenomenon 104.55 One mixing angle describes every neutral-current measurement ¶ ↺
- depends_on proposition 110.1 A pseudoscalar mean vanishes if parity holds ¶
  - depends_on equation 110.1 eq:expparity-P-map ¶
  - proves proof ch:12-exp-parity-violation@proof-1 ¶
- proves proof ch:12-exp-parity-violation@proof-14 ¶
proves proof ch:12-exp-parity-violation@proof-16 ¶

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type	direction	node	provenance	where
`cites` (data)	→	Precision measurement of the weak charge of the proton	derived	parts/11-qft-standard-model/12-exp-parity-violation.tex:1932
`depends_on`	→	One mixing angle describes every neutral-current measurement	declared	parts/11-qft-standard-model/12-exp-parity-violation.tex:1937
`depends_on`	→	Parity violation in electron scattering	declared	parts/11-qft-standard-model/12-exp-parity-violation.tex:1937
`proves`	←	ch:12-exp-parity-violation@proof-16	declared	parts/11-qft-standard-model/12-exp-parity-violation.tex:1940