Abstract
We develop here the general treatment of the Bethe-Salpeter equation for the bound state of two spin-1 particles interacting through an electromagnetic interaction. The treatment here, which can be generalized to strong interactions, combines the two-component approach utilized previously by the author in conjunction with spontaneous symmetry breaking. This is done by using a Lagrangian having SU(2) × U(1) symmetry (without fermions) and then choosing the 't Hooft gauge. In this way, a renormalizable theory for the interaction of two spin-1 particles via an electromagnetic interaction is ensured.
Original language | English |
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Pages (from-to) | 57-66 |
Number of pages | 10 |
Journal | Foundations of Physics |
Volume | 27 |
Issue number | 1 |
DOIs | |
State | Published - 1 Jan 1997 |
ASJC Scopus subject areas
- Philosophy
- General Physics and Astronomy
- History and Philosophy of Science