On parity conservation and neutrino mass
Author:
Publisher
Springer Science and Business Media LLC
Subject
Astronomy and Astrophysics,Nuclear and High Energy Physics,Atomic and Molecular Physics, and Optics
Link
http://link.springer.com/content/pdf/10.1007/BF02812841.pdf
Reference3 articles.
1. C. N. Yang andT. D. Lee. The author is indebted for a pre-print.
2. This is not the mass-reversal transformation discussed byJ. Tiomno (Nuovo Cimento,1, 226 (1955)) which requires invariance of the total Lagrangian when a substitutionψ →γ 5 ψ,m → −m is made for all fields. In this case neutrino self-mass δm v need not vanish. In fact δm v ∞mf(m 2) and thus $$\delta m_\nu \bar \psi _\nu \psi _\nu $$ does not change sign.
3. We write all field operators with their particle symbols: thusπ(x) stands for the π-meson field,v(x) for the neutrino-field etc.
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