Abstract
A relativistic nuclear Hamiltonian is constructed, from which the relativistic Hartree and Hartree-Fock equations are derived. Then the Hartree equations are applied to and nuclei taking as input different relativistic one-boson-exchange potentials as well as the effective interaction of Walecka, introduced in his theory of highly condensed matter. Single-particle energies turn out to be of the correct magnitude. In particular, it is possible to explain the magnitude of the spin-orbit splitting without any free parameter.
NUCLEAR STRUCTURE , ; calculated single-particle binding energies. Relativistic Hartree-Fock method.
- Received 1 September 1977
DOI:https://doi.org/10.1103/PhysRevC.18.1510
©1978 American Physical Society