A new effective Lagrangian for nuclear matter
arXiv:nucl-th/9608021 · doi:10.1016/S0370-2693(96)01433-5
Abstract
The relativistic mean field model, the Zimányi - Moszkowski (ZM) Lagrangian describes nuclear matter and stable finite nuclei even in the non-relativistic limit. It fails, however, to predict the correct non-relativistic spin-orbit (SO) coupling. In this paper we improve on this matter by an additional tensor coupling analogous to the anomalous gyromagnetic ratio. It can be adjusted to describe the SO-term without changing the mean field solution of the ZM-Lagrangian for nuclear matter.
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Cited by in corpus (5)
- The Nuclear Spin-Orbit Force in Chiral Effective Field Theories
- Large Lorentz Scalar and Vector Potentials in Nuclei
- Parametrisations of relativistic energy density functionals with tensor couplings
- New treatment of the chiral SU(3) quark mean field model
- Improved quark mass density- dependent model with quark-sigma meson and quark-omega meson couplings