Quick Search:
Author: Title/Abstract: Vol./No: Page:

Prog. Theor. Phys. Vol. 15 No. 5 (1956) pp. 445-460

[ Full Text PDF : FREE ACCESS (1170K) ]

Proposal for Experiments for Determination of Beta-Decay Interaction and Theory of Triple Cascade Transition

Masato Morita

Kobayasi Institute of Physical Research, Kokubunzi, Tokyo

(Received January 6, 1956)

Abstract:

Four new kinds of experiments on angular correlation in 3-, 5-(β 1st) or 6+(β 2nd) 4+1 2) 2+2 2)0+ are proposed so as to determine definitely ST (or VT) as the β-decay interaction. Some other decay schemes also useful for this purpose are discussed.
Various angular correlation functions are given for the successive triple transitions of α, β, γ rays and also of the other kind of particles.


URL : http://ptp.ipap.jp/link?PTP/15/445/
DOI : 10.1143/PTP.15.445

[ Full Text PDF : FREE ACCESS (1170K) ] Citation:


References:

  1. E. J. Konopinski, Rev. Mod. Phys. 27 (1955), 254[APS].
  2. B. M. Rustad and S. J. Raby, Phys. Rev. 89 (1953), 880[APS]; ibid. 97 (1955), 991[APS].
    J. S. Allen and W. K. Jentschke, Phys. Rev. 89 (1953), 902[APS].
  3. Maxson, Allen and Jentschke, Phys. Rev. 97 (1955), 109[APS].
    W. P. Alford and D. H. Hamilton, Phys. Rev. 95 (1954), 1351[APS].
  4. P. Macq, Bulletin de la Classe des Science, 5e Série XL (1954), 802
  5. D. T. Stevenson and M. Deutsch, Phys. Rev. 84 (1951), 1071[APS].
  6. H. Rose, Phil. Mag. 44 (1953), 739.
  7. D. T. Stevenson and M. Deutsch, Phys. Rev. 83 (1951), 1202[APS].
  8. I. Shaknov, Phys. Rev. 82 (1951), 333[APS].
  9. See reference 7), and E. K. Darby and W. Opechowski, Phys. Rev. 83 (1951), 676[APS].
  10. See reference 5).
  11. T. B. Novey, Phys. Rev. 78 (1950), 66[APS].
    H. Rose, Phil. Mag. 43 (1952), 1146.
  12. T. B. Novey, private communication and ANL-5523 (1956).
  13. T. Hayashi, private communication.
  14. Cork, LeBlanc, Nester, Martin and Brice, Phys. Rev. 90 (1953), 444[APS].
    G. L. Keister, L. B. Lee and F. H. Schmidt, Phys. Rev. 97 (1955), 451[APS].
  15. V. E. Krohn and S. Raboy, Phys. Rev. 97 (1955), 1017[APS].
  16. M. Sasaki, J. Phys. Soc. Jpn. 10 (1955), 729, [JPSJ]and private communication.
  17. L. C. Biedenharn, G. B. Arfken and M. E. Rose, Phys. Rev. 83 (1951), 586, [APS]abbreviated as BAR.
  18. For example, M. Morita, Prog. Theor. Phys. 14 (1955), 27, [PTP]abbreviated as M.
  19. Tables of Racah coefficient.
    L. C. Biedenharn et al., Oak Ridge National Laboratory Report ORNL 1098 (1953) and ORNL 1679 (1954).
    S. Obi et al., Ann. Tokyo Astro. Obs. Second Series III No. 3 (1953), 89; ibid. IV No. 1 (1955), 1; ibid. IV No. 2 (1955), 77.
  20. H. A. Tolhoek, and J. A. M. Cox, Physica, 19 (1953), 101[CrossRef].
    H. A. Tolhoek, Physica 19 (1953), 673[CrossRef].
    O. J. Poppema, J. G. Siekman, R. Van Wageningen and H. A. Tolhoek, Physica 21 (1955), 223[CrossRef].
    A. Simon, M. E. Rose and J. M. Jauch, Phys. Rev. 84 (1951), 1155[APS].
    N. R. Steenberg, Proc. R. Soc. A 65 (1952), 791; ibid. 66 (1953) 391; ibid. 66 (1953) 399; Phys. Rev. 93 (1954), 678[APS].
  21. M. Sasaki, H. Ogata and M. Morita, Physica in press.
  22. L. C. Biedenharn and M. E. Rose, Rev. Mod. Phys. 25 (1953), 729, [APS]abbreviated as BR.
  23. M. Ferentz and N. Rosenzweig, Argonne Mational Laboratory Report ANL-5324 (1955).
  24. M. Morita, Bulletin of Kobayasi Institute of Physical Research, 5 (1955) 123.
  25. R. W. King, Rev. Mod. Phys. 26 (1954), 327[APS].
  26. M. Nagasaki and T. Tamura, Prog. Theor. Phys. 12 (1954), 248[PTP].
  27. G. Scharff- Gordhaber and J. Weneser, Phys. Rev. 98 (1955), 212[APS].
  28. Keister et al., see reference 14).
  29. K. Siegbahn, Beta and Gamma Ray Spectroscopy (North-Holland Publishing Company, Amsterdam, 1955), p. 875, M. E. Rose's Table.
  30. M. Yamada, Prog. Theor. Phys. 10 (1953), 241[PTP].
    He verified this fact for the correction factors of β-spectra.
    Recently, he and Mr. Matumoto (private communication) showed to the author the same conclusions for the first forbidden transition without the restriction αZ ≪1.
    Study for bLL'(2n)'s is also proceeding by us.
  31. If we want to estimate the two corrections for bLL'(2n)'s explicitly, we should use FLL'M(θ) in terms of Li and Lij etc., which were given by us (see, references of M).