Relativistic Continuum Quasiparticle Random Phase Approximation in Spherical Nuclei
arXiv:1103.2332 · doi:10.1103/PhysRevC.83.044303
Abstract
We have calculated the strength distributions of the dipole response in spherical nuclei, ranging all over the periodic table. The calculations were performed within two microscopic models: the discretized quasiparticle random phase approximation (QRPA) and the quasiparticle continuum RPA, which takes into account the coupling of the single-particle continuum in an exact way. Pairing correlations are treated with the BCS model. In the calculations, two density functionals were used, namely the functional PC-F1 and the functional DD-PC1. Both are based on relativistic point coupling Lagrangians. It is explicitly shown that this model is capable of reproducing the giant as well as the pygmy dipole resonance for open-shell nuclei in a high level of quantitative agreement with the available experimental observations.
9 pages, 6 figures, accepted for publication in Phys. Pev. C
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- Low-energy dipole strength in 112,120Sn
- Systematic investigation of low-lying dipole modes using the canonical-basis time-dependent Hartree-Fock-Bogoliubov theory
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- Connecting the Pygmy Dipole Resonance to the neutron skin
- A self-consistent study of multipole response in neutron-rich nuclei using a modified realistic potential
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- Dipole response in neutron-rich nuclei with new Skyrme interactions
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