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Y. Nambu:Progr. Theor. Phys. (Kyoto),7, 595 (1952).
A good review of experimental tests of quantum electrodynamics is given byS. Drell: inAtomic Physics, edited byB. Bederson, V. Cohen andF. Pichanick (New York, 1969), p. 53.
M. H. Mac Gregor:Lett. Nuovo Cimento,4, 413, 1043 (1970).
M. H. Mac Gregor:Lett. Nuovo Cimento,4, 1309 (1970).
See, for example,L. B. Okun:Weak Interactions of Elementary Particles, Chap. 6 (London, 1965);J. Bernstein:Elementary Particles and Their Currents (San Francisco, 1968), p. 128.
J. A. Wheeler:Superspace, inAnalytical Methods in Mathematical Physics, edited byR. P. Gilbert andR. G. Newton (New York, 1970), p. 335.
M. H. Mac Gregor:Lett. Nuovo Cimento,4, 413 (1970).
M. H. Mac Gregor:Lett. Nuovo Cimento,4, 1249 (1970).
The values for the constants are fromB. N. Taylor, W. H. Parker andD. N. Langenberg:Rev. Mod. Phys.,41, 375 (1969).
All data for the meson systematics are fromM. Roos, C. Bricman, A. Barbaro-Galtieri, L. R. Price, A. Rittenberg, A. H. Rosenfeld, N. Barash-Schmidt, P. Söding, C. Y. Chien, C. G. Wohl andT. Lasinski:Phys. Lett.,33 B, 1 (1970).
J. P. Ostriker:Scientific American, January 1971, page 48.
See, for example,M. Schwarzschild:Structure and Evolution of the Stars, Chap. VII (Princeton, N. J., 1958).
In this model for the electron (ref. (8)), the radius must shrink dynamically under accelerations in order to conserve angular momentum. This shrinking can in a sense be seen experimentally. From the model (8), the magnetic moment of the electron is given by the equation μ=er/2, wheree is the electric charge andr is the radius of the electron. It has been accurately observed. (D. T. Wilkinson andH. R. Crane:Phys. Rev.,130, 852 (1963)).
SeeM. Ruderman:Scientific American, February 1971, page 24, for an interesting discussion of electron distributions in solids at high pressures (note the figures on page 27).
R. Ruffini andJ. A. Wheeler:Physics Today, January 1971, page 30. Page 19 of this issue also contains some new observational results on white dwarf stars.
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Mac Gregor, M.H. The fine-structure constant α=e 2/hc as a universal scaling factor. Lett. Nuovo Cimento 1, 759–764 (1971). https://doi.org/10.1007/BF02770123
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DOI: https://doi.org/10.1007/BF02770123