Abstract
A two-body Dirac equation is derived from quantum electrodynamics by consideration of crossed and uncrossed photon exchange. The equation is symmetric in the particle labels, and it reduces to the one-body Dirac equation when either particle's mass becomes infinite. The condition that negative-energy states must propagate backward in time is incorporated. Virtual pair contributions are taken into account to leading order in m-1 in a consistent and nonperturbative manner such that continuum dissolution cannot occur. A straightforward extension provides three-body and N-body equations.
| Original language | English |
|---|---|
| Pages (from-to) | 469-473 |
| Number of pages | 5 |
| Journal | Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics |
| Volume | 197 |
| Issue number | 4 |
| DOIs | |
| State | Published - 5 Nov 1987 |
| Externally published | Yes |
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