Abstract
When we treat an atom containing a number n of electrons by the method of the self-consistent field, we assume that each electron has its own particular “orbit,” specified by a wave function (q|r) in four variables q. These four variables are usually taken to be the three coordinates of the electron together with a variable describing the spin, but according to the transformation theory of quantum mechanics, they may be any four independent commuting functions of the coordinates, momenta and spin variables.
References
2
Referenced
119
- Proc. Camb. Phil. Soc. vol. xxvi, p. 376 (1930), equations (9), (10), (11).
10.1007/BF01340294
Dates
Type | When |
---|---|
Created | 16 years, 9 months ago (Nov. 7, 2008, 11:04 a.m.) |
Deposited | 6 years, 2 months ago (June 9, 2019, 3:23 p.m.) |
Indexed | 2 weeks, 6 days ago (Aug. 2, 2025, 12:33 a.m.) |
Issued | 94 years, 4 months ago (April 1, 1931) |
Published | 94 years, 4 months ago (April 1, 1931) |
Published Online | 16 years, 9 months ago (Oct. 24, 2008) |
Published Print | 94 years, 4 months ago (April 1, 1931) |
@article{Dirac_1931, title={Note on the Interpretation of the Density Matrix in the Many-Electron Problem}, volume={27}, ISSN={1469-8064}, url={http://dx.doi.org/10.1017/s0305004100010343}, DOI={10.1017/s0305004100010343}, number={2}, journal={Mathematical Proceedings of the Cambridge Philosophical Society}, publisher={Cambridge University Press (CUP)}, author={Dirac, P. A. M.}, year={1931}, month=apr, pages={240–243} }