Abstract

We discuss systematic global investigations with modern covariant density functionals. The number of their phenomenological parameters can be reduced considerable by using microscopic input from ab-initio calculations in nuclear matter. The size of the tensor force is still an open problem. Therefore we use the first full relativistic Brueckner-Hartree-Fock calculations in finite nuclear systems in order to study properties of such functionals, which cannot be obtained from nuclear matter calculations.

Highlights

  • In recent years important progress has been made in the ab-initio studies of nuclear properties

  • Because of the tremendously growing dimensions of the underlying configuration spaces the majority of heavy nuclei are, so far, only accessible through nuclear density functional theory (DFT)

  • We show results obtained in Relativistic Hartree-Fock (RHF)-calculations with the phenomenological effective interaction PKO1, which has been fitted to binding energies and charge radii of a set of spherical nuclei

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Summary

Introduction

In recent years important progress has been made in the ab-initio studies of nuclear properties. The Brueckner-Hartree-Fock (BHF) theory is one of the most promising theories for such a purpose It provides in a fully microscopic way a density dependent effective force for mean field calculations in nuclei. In the seventies much effort has been used to carry out such calculations in finite nuclei Such non-relativistic calculations usually failed to reproduce saturation, because of the missing three-body forces. The first full RHBF calculations have been carried out for finite nuclear systems [4, 5] They provide a basis to determine in future the size of the tensor forces in covariant density functionals on a microscopic basis

Phenomenological and Semi-microscopic CDFT’s
The problem of tensor forces
Microscopic RBHF calculations in finite nuclei
Findings
Conclusions
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