Advances in Computers, Vol. 17 by Marshall C. Yovits

By Marshall C. Yovits

Due to the fact that its first quantity in 1960, Advances in desktops has provided distinct assurance of ideas in and software program and in laptop thought, layout, and purposes. It has additionally supplied members with a medium within which they could research their matters in larger intensity and breadth than that allowed through typical magazine articles. therefore, many articles became ordinary references that stay of important, lasting price regardless of the swift development occurring within the box.

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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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