proposition 101.27 The sign and size of the cobalt asymmetry

open in the book · parts/11-qft-standard-model/03-weak-interactions.tex:1300 · p. 1956

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proposition 101.27: The sign and size of the cobalt asymmetry101.27equation 101.26: eq:weak-beta-asymmetry101.26proposition 101.32: Chirality and helicity in a state of definite momentum101.32proposition 101.34: The longitudinal polarization of a beta electron101.34experiment : Parity Violationexperime…proof : ch:03-weak-interactions@proof-19proofdefinition 101.29: Helicity101.29equation 101.30: eq:weak-chiral-projectors101.30phenomenon 103.64: Neutrinoless double beta decay has not been observed103.64proposition 101.38: The electron–neutrino correlation coefficients101.38proof : ch:03-weak-interactions@proof-22proofequation 101.31: eq:weak-chirality-weight101.31proof : ch:03-weak-interactions@proof-23proofproposition 105.20: Chirality and helicity105.20proposition 105.19: V-A violates parity maximally105.19proposition 101.15: Allowed selection rules101.15phenomenon 105.16: Beta emission from oriented nuclei is asymmetric105.16phenomenon 104.55: One mixing angle describes every neutral-current measurement104.55phenomenon 101.26: Parity is violated in weak decays101.26

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typedirectionnode provenancewhere
depends_on eq:weak-beta-asymmetry declared parts/11-qft-standard-model/03-weak-interactions.tex:1308
depends_on Chirality and helicity in a state of definite momentum declared parts/11-qft-standard-model/03-weak-interactions.tex:1308
depends_on The longitudinal polarization of a beta electron declared parts/11-qft-standard-model/03-weak-interactions.tex:1308
assumes Parity Violation declared parts/11-qft-standard-model/12-exp-parity-violation.tex:5
proves ch:03-weak-interactions@proof-19 declared parts/11-qft-standard-model/03-weak-interactions.tex:1312