The Dirac Electron in Simple Fields
- 1 August 1932
- journal article
- research article
- Published by American Physical Society (APS) in Physical Review B
- Vol. 41 (3), 278-290
- https://doi.org/10.1103/physrev.41.278
Abstract
The relativity wave equations for the Dirac electron are transformed in a simple manner into a symmetric canonical form. This canonical form makes readily possible the investigation of the characteristics of the solutions of these relativity equations for simple potential fields. If the potential is a polynomial of any degree in , a continuous energy spectrum characterizes the solutions. If the potential is a polynomial of any degree in , the solutions possess a continuous energy spectrum when the energy is numerically greater than the rest-energy of the electron; values of the energy numerically less than the rest-energy are barred. When the potential is a polynomial of any degree in , all values of the energy are allowed. For potentials which are polynomials in of degree higher than the first, the energy spectrum is again continuous. The quantization arising for the Coulomb potential is an exceptional case.
Keywords
This publication has 4 references indexed in Scilit:
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