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- W2181884380 abstract "The possibility to investigate the nuclear chart to the very limits of nuclear binding by new accelerators with radioactive beams has stimulated considerable new efforts on the theoretical side to understand the dynamics of the nuclear many-body problem by microscopic methods. Density functional theories (DFT) play a very important role in this context [1]. One of the underlying symmetries of QCD is Lorentz invariance and therefore covariant density functionals (CDFT) are of particular interest in nuclear physics [2,3] . This symmetry not only allows to describe the spin–orbit coupling in a consistent way, but it also puts stringent restrictions on the number of parameters in the corresponding functionals without reducing the quality of the agreement with experimental data. Therefore, a relatively small number of parameters is necessary, which are adjusted to reproduce a set of bulk properties of spherical nuclei. The resulting energy density functionals (EDF) are considered universal in the sense that they can be used for nuclei all over the chart of nuclides, where mean field is applicable, for ground state properties as well as for excited states. The most successful EDF originate from the Relativistic Hartree Bogoliubov (RHB) model in which p-h and p-p channels are treated simultaneously in a self-consistent manner. A large variety of nuclear phenomena have been described over the years within this model, the equation of state of symmetric nuclear matter, ground state properties of finite spherical and deformed nuclei at and far away from the valley of stability. The" @default.
- W2181884380 created "2016-06-24" @default.
- W2181884380 creator A5046251650 @default.
- W2181884380 date "2013-01-01" @default.
- W2181884380 modified "2023-09-27" @default.
- W2181884380 title "COVARIANT DENSITY FUNCTIONAL THEORY AND THE STRUCTURE OF EXOTIC NUCLEI" @default.
- W2181884380 hasPublicationYear "2013" @default.
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