Nonperturbative solution of two-body Dirac equations for quantum electrodynamics and related field theories.
Nonperturbative solution of two-body Dirac equations for quantum electrodynamics and related field theories.
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DOI:
10.1103/physrevd.46.5117
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发表时间:
1992-12
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影响因子:
--
通讯作者:
Crater;Becker;Wong;Van Alstine P
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文献类型:
--
作者:
Crater;Becker;Wong;Van Alstine P
In quark-model calculations of the meson spectrum, fully covariant two-body Dirac equations dictated by Dirac's relativistic constraint mechanics gave a good fit to the entire meson mass spectrum (excluding flavor mixing) with constituent world scalar and vector potentials depending on just one or two parameters. In this paper, we investigate the properties of these equations that made them work so well by solving them numerically for quantum electrodynamics (QED) and related field theories. The constraint formalism generates a relativistic quantum mechanics defined by two coupled Dirac equations on a 16-component wave function which contain Lorentz-covariant constituent potentials that are initially undetermined. An exact Pauli reduction leads to a second-order relativistic Schroedinger-like equation for a reduced eight-component wave function determined by an effective interaction---the quasipotential. We first determine perturbatively to lowest order the relativistic quasipotential for the Schroedinger-like equation by comparing that form with one derived from the Bethe-Salpeter equation. Insertion of this perturbative information into the minimal interaction structures of the two-body Dirac equations then completely determines their interaction structures.