- Autor(in)
- Referenz
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1 Fermi, E., Revs. Mod. Phys. 4 (1932) 87.
2 Vgl. z.B. Heisenberg, W., u. W. Pauli, Z. Phys. 56 (1929) 1;
3 Gupta, S., Proc. Phys. Soc. London A 63 (1950) 681;
4 Källen, G., Handb. d. Phys. (S. Flügge) Bd. 5, Teil 1, Springer-Verlag 1958.
5 Schmutzer, E., Relativistische Physik, Teubner-Verlag, Leipzig 1968.
6 Fock, V., und B. Podolsky, Z. Physik SU 1 (1932) 801.
Belinfante, F. J., Phys. Rev. 84 (1951) 644;
Bleuler, K., Helv. Phys. Acta 23 (1950) 567.
Coester, F., u. J. M. Jauch, Phys. Rev. 78 (1950) 149;
Proc. Phys. Soc. London A 64 (1951) 850;
Valatin, J. G., Dan. Mat. Fys. Medd. 26 (1951) Nr. 13.
- Seitenbereich
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0343 - 0352
- Zusammenfsg.
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The usual foundation of a covariant quantization of the M<small>AXWELL</small> field are the methods of F<small>ERMI</small> or B<small>LEULER</small> and G<small>UPTA</small> which lead to a series of difficulties and new problems. Here a new covariant method is proposed which uses directly the L<small>ORENTZ</small> condition.
- Artikel-Typen
- Forschungsartikel