I. Undor Calculus and Charge-Conjugation --; Zusammenfassung. Resumo --; ʹ 1. Introduction --; ʹ 2. The Dirac wave-function (undor of the first rank) --; ʹ 3. Charge-conjugation of four-spinors --; ʹ 4. Neutrettors of the first rank --; ʹ 5. Undors of the second rank --; ʹ 6. Covariant undor calculus --; References --; II. The Undor Equation of the Meson Field --; Zusammenfassung. Resumo --; ʹ 1. The Proca-Kemmer meson equation in undor notation --; ʹ 2. The generalized meson equation and the neutretto equation --; ʹ 3. The charge-conjugated meson equation --; ʹ 4. The charge current-density and the magnetic moment of mesons --; ʹ 5. Charge-invariance and statistics --; References --; III. The Heavy Quanta Theory of Nuclear and Cosmic Ray Phenomena --; ʹ 1. Introduction --; ʹ 2. The four types of meson fields proposed by Kemmer and the simplified deuteron problem --; ʹ 3. The charge-dependence of nuclear forces --; ʹ 4. Quantization and relativistic invariance of the theory --; ʹ 5. Elimination of the longitudinal electromagnetic field --; ʹ 6. Discussion of the Hamiltonian --; ʹ 7. The heavy quanta interaction between nuclons --; ʹ 8. The deuteron problem --; ʹ 9. The neutron-proton scattering --; ʹ 10. The spontaneous disintegration of heavy quanta. --; ʹ 11. The?-disintegration of instable nuclei --; ʹ 12. Scattering and absorption of mesons by nuclei --; ʹ 13. Discussion of the limits and the value of the theory --; References --; Samenvatting.
Grossen, we1che sich transformieren wie Produkte 4-komponentiger D ira c scher Wellenfunktionen, werden "Undoren" genannt. Zu jedem Undor tjJ kann durch Linearkombination der Komponenten seines kom plex Konjugierten tjJ* ein neuer "ladungskonjugierter" Undor tjJ£ gebil det werden. Wenn tjJ =