The spinor Bethe-Salpeter equation describing bound states of a fermion-antifermion pair with massless-boson exchange reduces to a single (uncoupled) partial differential equation for special combinations of the fermion-boson couplings. For spinless bound states with positive or negative parity this
Generalized Wilson expansions in dimensional renormalization: P. S. Collecott, Max-Planck-Institut für Physik und Astrophysik, Postfach 40 12 12, D-8000 München 40, Federal Republic of Germany
- Publisher
- Elsevier Science
- Year
- 1978
- Tongue
- English
- Weight
- 80 KB
- Volume
- 113
- Category
- Article
- ISSN
- 0003-4916
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✦ Synopsis
The spinor Bethe-Salpeter equation describing bound states of a fermion-antifermion pair with massless-boson exchange reduces to a single (uncoupled) partial differential equation for special combinations of the fermion-boson couplings. For spinless bound states with positive or negative parity this equation is a generalization to nonvanishing bound-state masses of the equations studied by Kummer and Goldstein, respectively. In the tight-binding limit the Kummer equation has a discrete spectrum, in contrast to the Goldstein equation, while for loose binding only the generalized Goldstein equation has a nonrelativistic limit. For intermediate binding energies the equations are solved numerically. The generalized Kummer equation is shown to possess a discrete spectrum of coupling constants for all bound-state masses. For the generalized Goldstein equation a discrete spectrum of coupling constants is found only if the binding energy is smaller than a critical value.
A Points-Splitting and Dimensional Renormalization.
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