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論文

Decay studies of the long-lived states in $$^{186}$$Tl

Stryjczyk, M.*; Andel, B.*; Andreyev, A. N.; Cubiss, J.*; Pakarinen, J.*; 他43名*

Physical Review C, 102(2), p.024322_1 - 024322_9, 2020/08

Decay spectroscopy of the long-lived states in $$^{186}$$Tl has been performed at ISOLDE, CERN. The $$alpha$$ decay from the low-spin (2$$^{-}$$) state in $$^{186}$$Tl was observed for the first time and a half-life was determined. Based on the $$alpha$$-decay energy, the relative positions of the long-lived states were fixed, with the (2$$^{-}$$) state as the ground state, the 7$$^{(+)}$$ state at 77(56) keV, and the 10$$^{(-)}$$ state at 451(56) keV. The level scheme of the internal decay of the $$^{186}$$Tl(10$$^{(-)}$$) state, which was known to decay solely through emission of 374-keV $$gamma$$-ray transition, was extended and a lower limit for the $$beta$$-decay branching b$$_{beta}$$ $$>$$ 5.9(3)% was determined. The extracted retardation factors for the $$gamma$$ decay of the 10$$^{(-)}$$ state were compared to the available data in neighboring odd-odd thallium isotopes indicating the importance of the $$pi$$d$$_{3/2}$$ shell in the isomeric decay and significant structure differences between $$^{184}$$Tl and $$^{186}$$Tl.

論文

Search for excited state of $$_{Sigma }^{4}{rm He}$$ hypernucleus in the J-PARC E13 experiment

中川 真菜美*; 長谷川 勝一; 早川 修平; 細見 健二; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; 田村 裕和; 谷田 聖; et al.

JPS Conference Proceedings (Internet), 26, p.023005_1 - 023005_3, 2019/11

The $$Sigma N$$ interaction is not much studied than the $$Lambda N$$ interaction. To understand the $$Sigma N$$ interaction, we study $$Sigma$$ hypernuclei. As for the $$Sigma$$ hypernucleus, only the ground state of $$_{Sigma }^{4}{rm He}$$ has been observed. To obtain more information about the $$Sigma N$$ interaction, the excited state should be studied. Therefore, we measure the missing-mass of the $$^4$$He$$(K^-,pi^-)$$ reaction at $$p_{K^-} = 1.5$$ GeV/$$c$$ and $$theta_{rm Lab} =$$ 2-14$$^{circ}$$ at the J-PARC K1.8 beam line. The ground state of $$_{Sigma }^{4}{rm He}$$ is observed whereas a peak of the excited states is not observed. We also observe suppression of the $$Sigma$$ quasi-free process at smaller angles.

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