Effects of Residual Tensor and Pairing Forces on the Gamow-Teller states in Magic Nuclei, <SUP>48</SUP>Ca, <SUP>90</SUP>Zr, <SUP>132</SUP>Sn, and <SUP>208</SUP>Pbopen accessEffects of Residual Tensor and Pairing Forces on the Gamow-Teller states in Magic Nuclei, 48Ca, 90Zr, 132Sn, and 208Pb
- Other Titles
- Effects of Residual Tensor and Pairing Forces on the Gamow-Teller states in Magic Nuclei, 48Ca, 90Zr, 132Sn, and 208Pb
- Authors
- Ha, Eunja; Cheoun, Myung-Ki; Sagawa, H.
- Issue Date
- Jun-2024
- Publisher
- Oxford University Press
- Citation
- Progress of Theoretical and Experimental Physics, v.2024, no.6, pp 1 - 15
- Pages
- 15
- Indexed
- SCIE
SCOPUS
- Journal Title
- Progress of Theoretical and Experimental Physics
- Volume
- 2024
- Number
- 6
- Start Page
- 1
- End Page
- 15
- URI
- https://scholarworks.bwise.kr/hanyang/handle/2021.sw.hanyang/197514
- DOI
- 10.1093/ptep/ptae077
- ISSN
- 2050-3911
2050-3911
- Abstract
- We investigate the effects of residual tensor force (TF) and pairing force on the Gamow-Teller (GT) transitions in four magic nuclei, Ca-48, Zr-90, Sn-132 and Pb-208. The TF is taken into account by using the Br & uuml;ckner G-matrix theory with the charge-dependent (CD) Bonn potential as the residual interaction of charge-exchange quasiparticle random phase approximation (QRPA). We found that particle-particle (p-p) tensor interaction does not affect the GT transitions because of the closed shell nature in the nuclei, but repulsive particle-hole (p-h) residual interaction for the p-h configuration of spin-orbit partners dominates the high-lying giant GT states for all of the nuclei. It is also shown that appreciable GT strengths are shifted to a lower energy region by the attractive p-h TF for the same j(pi) = j(nu) configuration, and produce the low-lying GT peak about 2.5 MeV in Ca-48. Simultaneously, in Zr-90 and Sn-132, the low-energy GT strength appears as a lower energy shoulder near the main GT peak. On the other hand, the shift of the low-lying GT state is not seen clearly for Pb-208 because of the strong spin-orbit splitting of high j orbits, which dominates the GT strength.
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