Abstract
The two-body covariant equation recently applied to QED problems is here generalized to N spin 1/2 particles interacting via the exchange of massless vector bosons and derived from an action principle. This is a nonperturbative one-time equation whose Hamiltonian is additive in the center of mass and relative variables. All recoil corrections and radiative effects are included. In this formulation, the relativistic many-body problem has the same structure as the Schrödinger many-body problem.
Full Text 
Sign-in/Register to access full text options
Sign-in/Register to access full text options 
Published version (
Free)
Free) 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a call
