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Published on: May 3, 2019
1p3/2 proton-hole state in 132Sn and the shell structure along N = 82
J Taprogge1, A Jungclaus2, H Grawe3
1Instituto de Estructura de la Materia, CSIC, E-28006 Madrid, Spain and Departamento de Física Teórica, Universidad Autónoma de Madrid, E-28049 Madrid, Spain and RIKEN Nishina Center, RIKEN, 2-1 Hirosawa, Wako-shi, Saitama 351-0198, Japan.
Researchers identified a new proton hole state in 131In, revealing an unexpected absence of proton subshell closures in N=82 isotones. This finding impacts understanding of the N=82 shell gap evolution in r-process nucleosynthesis.
Area of Science:
- Nuclear Physics
- Nuclear Structure
- Astrophysical Nucleosynthesis
Background:
- 132Sn is a doubly magic nucleus, serving as a reference for nuclear structure studies.
- Proton hole nuclei near 132Sn provide insights into nuclear shell effects and deviations from simple models.
- Understanding N=82 isotones is crucial for modeling the rapid neutron-capture (r-process) nucleosynthesis.
Purpose of the Study:
- To identify and characterize a new low-lying state in the 131In nucleus.
- To investigate the nuclear structure of experimentally inaccessible N=82 isotones below 132Sn.
- To explore the evolution of the N=82 shell gap in the context of the r-process.
Main Methods:
- Observation of gamma decay from a newly identified state in 131In.
- Populating the state via beta decay of 131Cd and beta-delayed neutron emission from 132Cd.
- Performing shell-model calculations using newly obtained experimental data.
Main Results:
- A new state in 131In was identified at an excitation energy of 1353 keV.
- This state is characterized as the previously unknown πp3/2 single-hole state relative to the 132Sn core.
- Shell-model calculations revealed a surprising lack of proton subshell closures in the N=82 isotone chain.
Conclusions:
- The identified πp3/2 single-hole state in 131In provides critical experimental data for nuclear structure models.
- The absence of predicted proton subshell closures challenges current nuclear structure theories for this region.
- This finding has significant implications for the predicted N=82 shell gap evolution and r-process element abundances.
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