Hostname: page-component-586b7cd67f-t8hqh Total loading time: 0 Render date: 2024-11-28T08:39:24.233Z Has data issue: false hasContentIssue false
  • English
  • Français

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

Published online by Cambridge University Press:  14 February 2012

Kathleen Sarginson
Get access Rights & Permissions [Opens in a new window]

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

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

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