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Beta-decay study of Tz = - 2 proton-rich nucleus 24Si
Authors:Y Ichikawa  T Kubo  N Aoi  V Banerjee  A Chakrabarti  N Fukuda  H Iwasaki  S Kubono  T Motobayashi  T Nakabayashi  T Nakamura  T Nakao  T Okumura  H J Ong  T K Onishi  D Suzuki  H Suzuki  M K Suzuki  T Teranishi  K N Yamada  H Yamaguchi  H Sakurai
Institution:1. Department of Physics, University of Tokyo, 7-3-1 Hongo, Bunkyo, 113-0033, Tokyo, Japan
2. RIKEN Nishina Center, RIKEN, 2-1 Hirosawa, Wako, 351-0198, Saitama, Japan
3. Variable Energy Cyclotron Centre, 1/AF, Bidhan Nagar, 700 064, Kolkata, India
4. Center for Nuclear Study, University of Tokyo, 7-3-1 Hongo, Bunkyo, 113-0033, Tokyo, Japan
5. Department of Physics, Tokyo Institute of Technology, 2-12-1 Oh-okayama, Meguro, 152-8551, Tokyo, Japan
6. Department of Physics, Kyushu University, 6-10-1 Hakozaki, Higashi, 812-8581, Fukuoka, Japan
Abstract: $ \beta$ -decay spectroscopy on a T z = - 2 proton-rich nucleus 24Si was performed. The decay scheme of 24Si was reconstructed by the $ \beta$ -delayed $ \gamma$ -ray and proton measurements. Two $ \beta$ branches to the bound 11 + and 12 + states in 24Al were observed for the first time. The observation of the allowed transition firmly established the spin-parity assignment for the 12 + states. The branching ratios to the 11 + and 12 + states were determined to be 31(4)% and 23.9(15)%, respectively. The branching ratios to three unbound states in 24Al including a new level at 6.735MeV were also determined for the first time. The level structure of 24Al was compared with its mirror nucleus 24Na . The Thomas-Ehrman shift on the 12 + state indicates s -wave dominance in the state as well as a characteristic behavior of the weakly bound s -wave proton in 24Al .
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