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VIII.—Reciprocity. Part VI: The Wave Function of the Meson

Published online by Cambridge University Press:  14 February 2012

Kathleen Sarginson
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Extract

In this paper the equations of the meson are treated in the same manner as the Dirac equation in a previous paper (K. Fuchs, 1940, Part IV). We use the formulae developed by Kemmer (1939), with a small modification, introduced so that the set of Maxwell's equations for the electro-magnetic field is obtained as a special case.

Type
Research Article
Information
Proceedings of the Royal Society of Edinburgh Section A: Mathematics , Volume 61 , Issue 1 , 1941 , pp. 77 - 92
Copyright
Copyright © Royal Society of Edinburgh 1941

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References

References to Literature

Born, M., 1939. “Reciprocity. Part I,” Proc. Roy. Soc. Edin., vol. lix, p. 219.Google Scholar
Born, M., and Fuchs, K., 1940. “Reciprocity. Parts II and I II,” Proc. Roy. Soc. Edin., vol. Ix, pp. 100, 141.Google Scholar
Fuchs, K., 1940, 1941. “Reciprocity. Parts IV and V,” Proc. Roy. Soc. Edin., vol. lx, p. 147; vol. lxi, p. 26.CrossRefGoogle Scholar
Kemmer, N., 1939. Proc. Roy. Soc, A, vol. clxxiii, p. 91.Google Scholar
Fröhlich, H., Heitler, W., and Kemmer, N., 1938. Proc. Roy. Soc, A, vol. clxvi, p. 154.Google Scholar