期刊
PHYSICAL REVIEW C
卷 104, 期 2, 页码 -出版社
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevC.104.024318
关键词
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资金
- JSPS KAKENHI [JP19K03824, JP19K03872]
This study aims to uncover the microscopic mechanism for the appearance of low-energy 2(-) state in Cf-248, as well as investigate the possible occurrence of the low-energy K-pi = 2(+) state, highlighting the need for improvements in EDFs to describe pairing correlations and shell structures in heavy nuclei.
Background: Rotational bands have been measured around Fm-250 associated with strong deformed-shell closures. The K-pi = 2(-) excited band emerges systematically in N = 150 isotones raging from plutonium to nobelium with even-Z numbers, and a sharp drop in energies was observed in californium. Purpose: I attempt to uncover the microscopic mechanism for the appearance of such a low-energy 2(-) state in Cf-248. Furthermore, I investigate the possible occurrence of the low-energy K-pi = 2(+) state, the. vibration, to elucidate the mechanism that prefers the simultaneous breaking of the reflection and axial symmetry to the breaking of the axial symmetry alone in this mass region. Method: I employ a nuclear energy-density functional (EDF) method: the Skyrme-Kohn-Sham-Bogoliubov and the quasiparticle random-phase approximation are used to describe the ground state and the transition to excited states. Results: The Skyrme-type SkM* and SLy4 functionals reproduce the fall in energy but not the absolute value of the K-pi = 2(-) state at Z = 98 where the proton two-quasiparticle excitation [633]7/2 circle times [521]3/2 plays a decisive role for the peculiar isotonic dependence. I find interweaving roles by the pairing correlation of protons and the deformed-shell closure at Z = 98. The SkM* model predicts the K-pi = 2(-) state appears lower in energy in Cf-246 than in 248Cf as the Fermi level of neutrons is located in between the [622]5/2 and the [734]9/2 orbitals. Except for Fm-250 in the SkM* calculation, the Kp = 2(+) state is predicted to appear higher in energy than the K-pi = 2(+) state because the quasiproton [521]1/2 orbital is located above the [633]7/2 orbital. Conclusions: A systematic study of low-lying collective states in heavy actinide nuclei provides a rigorous testing ground for microscopic nuclear models. The present paper shows a need for improvements in the EDFs to describe pairing correlations and shell structures in heavy nuclei, that are indispensable in predicting the heaviest nuclei.
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