Advances Electronics and Electron Physics. Vol. XI by L. Marton

By L. Marton

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E. Taft and L. Apker, J . Opt. Soc. Am. 43, 81 (1953). 27. W. Kluge, 2. Physik 67,497 (1931). 88. W. J. Turner, Phys. Rev. 101, 1653 (1956). 29. P. Gorlich, Arbeitstagung Biophys. Greifswald (1953); V. Schwetzoff, Rev. gin. elec. 63, (1954). SO. P. Gorlich, Ann. Physik [5] 13, 831 (1932); H. E. Hinteregger and K. Watanabe, J. Opt. Am. 43, 604 (1953). S1. D. W. Turner, Nature 179, 1022 (1957). 32. H. E. Hinteregger, Phys. Rev. 96,538 (1954); W. C. Walker, N. Wainfan, and G. L. Weissler, J . Appl.

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 [6], 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 [6] 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.

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