Abstract
A six-component theory of the vector field is proposed. An antisymmetric tensor second rank is used as the field function. The theory is invariant with respect to groups of dual transformations. The equations of motion are hyperbolic and causal when the electromagnetic interaction is included.
Similar content being viewed by others
Literature cited
A. Proca, J. Phys. Rad.,7, 347 (1936).
J. Takahashi and R. Palmer, Phys, Rev.,D1, 2947 (1970).
D. Shay and R. Good, Phys. Rev.,179, 1410 (1969).
S. Weinberg, Phys. Rev.,B133, 1318 (1964).
A. Aurilia and H. Umezawa, Phys. Rev.,182, 1682 (1969).
A. Borgardt and D. Karpenko, Preprint ITF-72-105R [in Russian], Kiev (1972).
G. Velo and D. Zwanziger, Phys. Rev.,188, 2218 (1969).
T. Lee and C. Yang, Phys. Rev.,128, 885 (1962).
F. Rohrlich, Phys. Rev.,80, 666 (1950).
O. M. Boyarkin, Zh. Eksp. Teor. Fiz.,75, 26 (1978).
Author information
Authors and Affiliations
Additional information
Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 11, pp. 29–32, November, 1981.
Rights and permissions
About this article
Cite this article
Boyarkin, O.M. Dually invariant theory of particles of spin 1. Soviet Physics Journal 24, 1003–1005 (1981). https://doi.org/10.1007/BF00892501
Received:
Revised:
Issue Date:
DOI: https://doi.org/10.1007/BF00892501