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Exotic structure of the third excited state in^(21)Na
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作者 LI Xihan1,2,3, LIANG Yujie1,2,3, DENG Fuguo1,2,3, LIU Zuhua1,4 & ZHOU Hongyu1,2,3 1. Key Laboratory of Beam Technology and Material Modification of Minister of Education, beijing Normal University, beijing 100875, china 2. Institute of Low Energy Nuclear Physics, and Department of Material Science and Engineering, beijing Normal University, beijing 100875, china +1 位作者 3. beijing radiation center, beijing 100875, china 4. china Institute of Atomic Energy, beijing 102413, china 《Chinese Science Bulletin》 SCIE EI CAS 2005年第23期2677-2680,共4页
The probability of the last proton being out of the binding potential, P and the root-mean-square (rms) ra- dius (<r2>1/2= of the third excited state in 21Na are calcu- lated by means of asymptotic normalization... The probability of the last proton being out of the binding potential, P and the root-mean-square (rms) ra- dius (<r2>1/2= of the third excited state in 21Na are calcu- lated by means of asymptotic normalization coefficient (ANC) method with the experimental date existing. The results are P=54.73% and <r2>1/2=5.28 fm respectively. The P value and the contribution of the asymptotic part to the <r2>1/2 are compared with those of several other low energy states in 21Na. It is found that the valence particle in the third excited state has an obvious larger P than those of other states. The density distribution of the valence proton in this state is also compared with the nucleons in the nuclear core 20Ne, and a far extended tail can be seen clearly. These results show that the third ex- cited state in 21Na is a proton halo state. 展开更多
关键词 第三激发态 外部结构 有效半径 密度分布 渐近标准化系数
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