proposition 101.32 Chirality and helicity in a state of definite momentum

open in the book · parts/11-qft-standard-model/03-weak-interactions.tex:1552 · p. 1959

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proposition 101.32: Chirality and helicity in a state of definite momentum101.32definition 101.29: Helicity101.29equation 101.30: eq:weak-chiral-projectors101.30phenomenon 103.64: Neutrinoless double beta decay has not been observed103.64proposition 101.27: The sign and size of the cobalt asymmetry101.27proposition 101.38: The electron–neutrino correlation coefficients101.38proof : ch:03-weak-interactions@proof-22proofphenomenon 101.28: Neutrinos are left-handed101.28proposition 101.31: Chirality against helicity101.31proposition 101.35: The V-A current is the left-chiral current101.35equation 103.65: eq:flavour-mbetabeta103.65phenomenon 107.72: Double beta decay107.72proof : ch:05-flavour-neutrinos@proof-33proofequation 101.26: eq:weak-beta-asymmetry101.26proposition 101.34: The longitudinal polarization of a beta electron101.34experiment : Parity Violationexperime…proof : ch:03-weak-interactions@proof-19proofequation 101.37: eq:weak-enu-correlation101.37proof : ch:03-weak-interactions@proof-26proof

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typedirectionnode provenancewhere
depends_on Helicity declared parts/11-qft-standard-model/03-weak-interactions.tex:1569
depends_on eq:weak-chiral-projectors declared parts/11-qft-standard-model/03-weak-interactions.tex:1569
depends_on Neutrinoless double beta decay has not been observed declared parts/11-qft-standard-model/05-flavour-neutrinos.tex:3132
depends_on The sign and size of the cobalt asymmetry declared parts/11-qft-standard-model/03-weak-interactions.tex:1308
depends_on The electron–neutrino correlation coefficients declared parts/11-qft-standard-model/03-weak-interactions.tex:1819
proves ch:03-weak-interactions@proof-22 declared parts/11-qft-standard-model/03-weak-interactions.tex:1572