journal article
Aug 01, 1968
Exact solution of the Dirac-Pauli equation for a class of fields: Precession of polarization
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References
8
[1]
D. M. Volkov:Zeits. Phys.,94, 250 (1935).
10.1007/bf01331022
[2]
L. S. Brown andT. W. B. Kibble:Phys. Rev.,133, A 705 (1964);A. I. Nikishov andV. I. Ritus:Sov. Phys. JETP,19, 529 (1964);Žurn. Ėksp. Teor. Fiz.,46, 776 (1963));N. D. Sen Gupta:Zeits. Phys.,201, 222 (1961).P. J. Redmond:Jour. Math. Phys.,6, 1163 (1965). Many other relevant sources are quoted in the above three references.
10.1103/physrev.133.a705
[3]
V. Bargmann, L. Michel andV. L. Telegdi:Phys. Rev. Lett.,2, 435 (1959). (More details are given in the unpublished seminar notes ofL. Michel (1959)).
10.1103/physrevlett.2.435
[4]
A. Chakrabarti:Nuovo Cimento,43 A, 576 (1966).
10.1007/bf02756681
[5]
S. I. Rubinow andJ. B. Keller:Phys. Rev.,131, 2789 (1963);M. Kolsrud:Nuovo Cimento,39, 504 (1965);E. Plahte:Suppl. Nuovo Cimento,4, 246 (1966);P. Nyborg:Nuovo Cimento,31, 1209 (1964);H. Bacry:Ann. de Phys.,8, 197 (1963). Many other sources are quoted in these articles.
10.1103/physrev.131.2789
[6]
P. A. M. Dirac:Rev. Mod. Phys.,21, 392 (1949);34, 592 (1962).
10.1103/revmodphys.21.392
[7]
G. N. Fleming:Journ. Math. Phys.,7, 1959 (1966).
10.1063/1.1704880
[8]
Since τ=u·x, the relation (3.3) indicates thatu must be expressible in the form ((n·u)−1 n+σ) where σ·x=0 and the spacelike σ restoresu 2=1. The implicit forms obtained for the trajectory makes the explicit verification of the above fact rather difficult. The calculation leading to (3.3) is however very transparent, leaving no ambiguity possible.
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Details
- Published
- Aug 01, 1968
- Vol/Issue
- 56(3)
- Pages
- 604-624
- License
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Cite This Article
A. Charkrabarti (1968). Exact solution of the Dirac-Pauli equation for a class of fields: Precession of polarization. Il Nuovo Cimento A, 56(3), 604-624. https://doi.org/10.1007/bf02819823
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