The Dirac electron theory

[1] [Anonymous], 1930, QUANTUM MECH

[2] BATEMAN H, 1932, PARTIAL DIFFERENTIAL, pCH6

[3] Bechert K, 1930, ANN PHYS-BERLIN, V6, P700

[4] BECKER R, THEORIE ELEKT, V2, P124

[5] BECKER R, 1933, THEORIE ELEKT, V2

[6] BETHE, HDB PHYS, V24, P375

[7] About the interaction of two electrons. [J]. ZEITSCHRIFT FUR PHYSIK, 1932, 77 (5-6): : 296 - 306

[8] BETHE H, HDB PHYS, V24, P316

[9] Nuclear physics A. Stationary states of nuclei [J]. REVIEWS OF MODERN PHYSICS, 1936, 8 (02) : 0082 - 0229

[10] A possible explanation of the relativity doublets and anomalous Zeeman effect by means of a magnetic electron [J]. PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 1926, 12 : 80 - 85

[1] [Anonymous], 1930, QUANTUM MECH

[2] BATEMAN H, 1932, PARTIAL DIFFERENTIAL, pCH6

[3] Bechert K, 1930, ANN PHYS-BERLIN, V6, P700

[4] BECKER R, THEORIE ELEKT, V2, P124

[5] BECKER R, 1933, THEORIE ELEKT, V2

[6] BETHE, HDB PHYS, V24, P375

[7] About the interaction of two electrons. [J]. ZEITSCHRIFT FUR PHYSIK, 1932, 77 (5-6): : 296 - 306

[8] BETHE H, HDB PHYS, V24, P316

[9] Nuclear physics A. Stationary states of nuclei [J]. REVIEWS OF MODERN PHYSICS, 1936, 8 (02) : 0082 - 0229

[10] A possible explanation of the relativity doublets and anomalous Zeeman effect by means of a magnetic electron [J]. PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 1926, 12 : 80 - 85