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EC and $$alpha$$ decays of $$^{235}$$Am

$$^{235}$$AmのEC及び$$alpha$$崩壊

浅井 雅人 ; 阪間 稔*; 塚田 和明 ; 市川 進一; 羽場 宏光*; 西中 一朗; 永目 諭一郎; 後藤 真一*; 小島 康明*; 大浦 泰嗣*; 中原 弘道*; 柴田 理尋*; 河出 清*

Asai, Masato; Sakama, Minoru*; Tsukada, Kazuaki; Ichikawa, Shinichi; Haba, Hiromitsu*; Nishinaka, Ichiro; Nagame, Yuichiro; Goto, Shinichi*; Kojima, Yasuaki*; Oura, Yasuji*; Nakahara, Hiromichi*; Shibata, Michihiro*; Kawade, Kiyoshi*

$$^{235}$$AmのEC及び$$alpha$$崩壊を$$gamma$$線核分光の手法により調べた。$$^{235}$$Puの励起準位を初めて構築し、予備的ではあるが準位のスピン・パリティ及びニールソン軌道を同定した。実験結果から$$^{235}$$Amの基底状態の軌道配位を$$pi5/2^{-}[523]$$と評価した。一方$$^{231}$$Npの$$pi5/2^{-}[523]$$準位のエネルギーは15keV以下であることがわかり、実験で得られた$$alpha$$線のエネルギー値と合わせて、$$^{235}$$Amの$$Q_{alpha}$$値を6569$$^{+27}_{-12}$$keVと決定した。

EC and $$alpha$$ decays of $$^{235}$$Am have been studied by means of $$gamma$$-ray spectroscopy. Excited states in $$^{235}$$Pu have been established for the first time, and tentative spin-parity and Nilsson assignments were given to these levels. The ground state of $$^{235}$$Am was evaluated to be the $$pi 5/2^{-}[523]$$ state from the experimental results. It was found that the $$pi 5/2^{-}[523]$$ state in $$^{231}$$Np is located at $$<$$15~keV, which allowed us to determine the $$Q_{alpha}$$ value of $$^{235}$$Am as 6569$$^{+27}_{-12}$$~keV, in combination with the measured $$alpha$$-particle energy.

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パーセンタイル:49.41

分野:Physics, Nuclear

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