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The quantum theory of the Electron. Part II
Open accessAbstract
In a previous paper by the author* it is shown that the general theory of quantum mechanics together with relativity require the wave equation for an electron moving in an arbitrary electromagnetic field of potentials, A0, A1, A2, A3 to be of the form FΨ ≡ [p0 e / c A0 + α1 (p1 + e / c A1) + α2 (p2 + e / c A2) + α3(p3 + e / c A3) + α4mc] Ψ = 0. (1) The α’s are new dynamical variables which it is necessary to introduce in order to satisfy the conditions of the problem. They may be regarded as describing some internal motion of the electron, which for most purposes may be taken to be the spin of the electron postulated in previous theories. We shall call them the spin variables.
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Cited by
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Dirac, Majorana, and Weyl fermions
Pal, P. B. (2011) · American Journal of Physics · doi:10.1119/1.3549729 · Cited by 230
Oscillatory multiband dynamics of free particles: The ubiquity of zitterbewegung effects
Winkler, R., Zülicke, U., & Bolte, J. (2007) · Physical Review B · doi:10.1103/physrevb.75.205314 · Cited by 70
Merkl, M., Zimmer, F. E., Juzeliūnas, G., & Öhberg, P. (2008) · EPL (Europhysics Letters) · doi:10.1209/0295-5075/83/54002 · Cited by 64
Semiclassical dynamics and transport of the Dirac spin
Chuu, C.-P., Chang, M.-C., & Niu, Q. (2010) · Solid State Communications · doi:10.1016/j.ssc.2009.10.039 · Cited by 40
Metadata
- Authors
- Dirac, P. A. M.
- Venue
- Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character
- Publisher
- The Royal Society
- Published
- 1928-03-01
- Volume
- 118
- Issue
- 779
- Pages
- 351-361
- ISSN
- 0950-1207 (ISSN-L)
- 2053-9150
- OpenAlex
- W2023814380
- Cited by
- 715
- References
- 0
- FWCI
- 4.83
- Type
- journal article
- Language
- en
- Open access
- diamond
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- Dirac, P. A. M. (1928). The quantum theory of the Electron. Part II. Proceedings of the Royal Society of London. Series A, Containing Papers of a Mathematical and Physical Character. https://doi.org/10.1098/rspa.1928.0056
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