Electromagnetic effects and precision mass calculations

Part IV. Refinements and Ramifications
Part of the Lecture Notes in Physics book series (LNP, volume 81)


Uranium Reso Prolate 
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References for Chapter 19

  1. 1.
    See B. T. Feld, Models of Elementary Particles, Blaisdell, Waltham (1969), page 339, Eq. 18a'.Google Scholar
  2. 2.
    T. G. Trippe et al., Review of Particle Properties, Rev. Mod. Phys. 48, No. 2 Part II, April 1976. A more recent value for the Σ− magnetic moment is quoted in G. Dugan et al., Nucl. Phys. A254, 396 (1975),which is in essential agreement with the value The value listed here for the Σ+ magnetic moment is a new “world average,” including new data, that is reported by N. Doble et al., Phys. Lett. 67B, 483 (1977); these authors point out that this large value, when combined with the values for the A and p magnetic moments, raises some real problems with the SU(3) calculations. (See Ref. 10 for the A magnetic moment.)Google Scholar
  3. 3.
    See M. H. MacGregor, Nuovo Cimento 36A, 113 (1976).Google Scholar
  4. 4.
    A Zee, Physics Reports 3C, 127 (1972); see the references that are cited in this review article on the problem of the n-p mass difference.Google Scholar
  5. 5.
    J. L. Rosner, Physics Reports 11C, 189 (1974); see page 219.Google Scholar
  6. 6.
    M. Beg et al., Phys. Rev. Lett. 13, 514 (1964).Google Scholar
  7. 7.
    See Table 15.10 on page 340 of Ref. 1.Google Scholar
  8. 8.
    See Table 15.11 on page 341 of Ref. 1.Google Scholar
  9. 9.
    L. B. Rédei, Phys. Rev. D2, 239 (1970).Google Scholar
  10. 10.
    The Λ magnetic moment value listed in Table 19.6 is the new “world average” as given in RPP78. It includes recent measurements by G. Bunce et al., Phys. Rev. Lett. 36, 1113 (1976), and by K.Heller et al., Phys. Lett. 68B, 480 (1977).Google Scholar

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© Springer-Verlag 1978

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