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A Theoretical Study of Photoabsorption Cross Sections of Na^+ 2
引用本文:张卫华,高翔,韩小英,李家明.A Theoretical Study of Photoabsorption Cross Sections of Na^+ 2[J].中国物理快报,2007,24(8):2230-2233.
作者姓名:张卫华  高翔  韩小英  李家明
作者单位:[1]Key Laboratory of Atomic and Molecular Nanosciences of Ministry of Education, Department of Physics, Tsinghua University, Beijing 100084 [2]Department of Physics, Shanghai Key Laboratory for Laser Fabrication and Material Science, Shanghai Jiao Tong University, Shanghai 200030
摘    要:In the framework of quantum defect theory, we calculate photoabsorption cross sections of Na^+ 2. Based on our calculations, there is an absorption window in the photoabsorption cross sections of Na^+ 2. and more than one bump above the absorption window. The calculated photoabsorption cross sections provide an explanation for the abnormal bump in the experimental measurements of Hudson, which is a long-standing experimental puzzle.

关 键 词:光吸收    中子  原子核  截面
收稿时间:2007-1-25
修稿时间:2007-01-25

A Theoretical Study of Photoabsorption Cross Sections of Na2+
ZHANG Wei-Hua,GAO Xiang,HAN Xiao-Ying,LI Jia-Ming.A Theoretical Study of Photoabsorption Cross Sections of Na2+[J].Chinese Physics Letters,2007,24(8):2230-2233.
Authors:ZHANG Wei-Hua  GAO Xiang  HAN Xiao-Ying  LI Jia-Ming
Affiliation:1. Key Laboratory of Atomic and Molecular Nanosciences of Ministry of Education, Department of Physics, Tsinghua University, Beijing 100084 ; 2 Department of Physics, Shanghai Key Laboratory for Laser Fabrication and Material Science, Shanghai Jiao Tong University, Shanghai 200030
Abstract:In the framework of quantum defect theory, we calculate photoabsorptioncross sections of Na2+. Based on our calculations, there is an absorption window in the photoabsorption cross sections of Na2+, and more than one bump above the absorption window. The calculated photoabsorption cross sections provide an explanation for the abnormal bump in the experimental measurements of Hudson, which is a long-standing experimental puzzle.
Keywords:33  20  -t  33  70  Ca  33  80  Eh  31  15  Ne
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