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Extra info for Advances Electronics and Electron Physics. Vol. XI
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V. , Progr. Phys. Sci. ) 69,371 (1956). 20. A. L. Hughes and L. A. ” McGraw-Hill, New York, 1932. 21. P. Gorlich, 2. Physik 116, 704 (1940); A. Lallemand and M. Duchesne, 2. angew. Math. u. Phys. 1, 195 (1950); F. Eckart, Ann. Physik , 16,322 (1955). 22. S. Asao, Proc. Math. J a p a n 22, 448 (1940); P. G. Borsjak, J . Tech. Phys. ) 20, 928 (1950); Repts. Acad. Sci. Ukr. R. p. 330 (1956). 2s. F. Eckart, Ann. Physik  16, 322 (1955); K. Mikke, Elektronika 3, No. 2/3, 3 (1957). 24. Ba0: H. B.
For zero spin, the parity of the e is P, = +l, and hence e and r cannot be alternate decay modes of the same particle ( K meson), unless parity is not conserved in the decay interaction. In this case, the parity of the T+ can be decided by determining the fraction of nearzero energy pions in a large number of rf meson decays. A more detailed argument shows that: 1. If there exists a zero-energy pion (T+or s-) in the 3s state of r-decay and if parity is conserved in the decay, then e and r are different particles.