Gauging the three-nucleon spectator equation
arXiv:nucl-th/9706052 · doi:10.1103/PhysRevC.56.2973
Abstract
We derive relativistic three-dimensional integral equations describing the interaction of the three-nucleon system with an external electromagnetic field. Our equations are unitary, gauge invariant, and they conserve charge. This has been achieved by applying the recently introduced gauging of equations method to the three-nucleon spectator equations where spectator nucleons are always on mass shell. As a result, the external photon is attached to all possible places in the strong interaction model, so that current and charge conservation are implemented in the theoretically correct fashion. Explicit expressions are given for the three-nucleon bound state electromagnetic current, as well as the transition currents for the scattering processes γHe3 -> NNN, Nd -> γNd, and γHe3 -> Nd. As a result, a unified covariant three-dimensional description of the NNN-γNNN system is achieved.
23 pages, REVTeX, epsf, 4 Postscript figures
References in corpus (1)
Cited by in corpus (19)
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- Electromagnetic Structure of Few-Nucleon Ground States
- Gauging of equations method. I. Electromagnetic currents of three distinguishable particles
- A covariant view on the nucleons' quark core
- Gauging of equations method. II. Electromagnetic currents of three identical particles
- Electromagnetic interactions of three-body systems in the covariant spectator theory
- Gauging the spectator equations
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- First results for electromagnetic three-nucleon form factors from high-precision two-nucleon interactions
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- Covariant equations for the tetraquark and more
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- Generalized parton distributions for dynamical equation models
- Unified relativistic description of piNN and gamma-piNN
- Renormalisation-group analysis of electromagnetic couplings in the pionless effective field theory
- Conserved electromagnetic currents in a relativistic optical model
- Removal of singularities from the covariant spectator theory
- Gauge invariant formulation of 3 decay of particle-antiparticle bound states