Relativistic pionic effects in quasielastic electron scattering
arXiv:nucl-th/0106035 · doi:10.1016/S0375-9474(01)01253-2
Abstract
The impact of relativistic pionic correlations and meson-exchange currents on the response functions for electromagnetic quasielastic electron scattering from nuclei is studied in detail. Results in first-order perturbation theory are obtained for one-particle emission electronuclear reactions within the context of the relativistic Fermi gas model. Improving upon previous analyses where non-relativistic reductions of the currents were performed, here a fully relativistic analysis in which both forces and currents are treated consistently is presented. Lorentz covariance is shown to play a crucial role in enforcing the gauge invariance of the theory. Effects stemming uniquely from relativity in the pionic correlations are identified and, in particular, a comprehensive study of the self-energy contributions and of the currents associated with the pion is presented. First- and second-kind scaling for high momentum transfer is investigated.
43 pages, 21 figures
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- Superscaling in dilute Fermi gas and its relation to general properties of the nucleon momentum distribution in nuclei
- Crossing symmetry and phenomenological widths in effective Lagrangian models of the pion photoproduction process
- Longitudinal and Transverse Scaling Functions within the Coherent Density Fluctuation Model
- Superscaling in electron- and neutrino-nucleus scattering
- Fermion propagators in space-time
- Superscaling of non-quasielastic electron-nucleus scattering