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机构地区:[1]西北师范大学物理与电子工程学院,兰州730070
出 处:《物理学报》2007年第7期3887-3892,共6页Acta Physica Sinica
基 金:国家自然科学基金(批准号:10376026;10434100);兰州重离子加速器国家实验室原子核理论中心基金;科技部国际合作项目(批准号:CI-2004-07)资助的课题.~~
摘 要:在分析双洞相关退激发对双洞态退激发的贡献较小的基础上,依据辐射-俄歇-双俄歇级联退激发模型(RACDA)研究了Mg1+(1s-1)(K壳层单洞态镁离子)和Mg2+(1s-2)(K壳层双洞态镁离子)的退激发过程,计算了它们的末电离态离子的分布,并与辐射-俄歇级联退激发模型的结果进行了比较.RACDA模型计算的Mg1+(1s-1)的4价末电离态离子的相对丰度较大,而辐射-俄歇级联退激发模型(RAC)的结果中就没有出现4价离子;两种模型计算Mg2+(1s-2)的6价末电离态离子的丰度非常大,而RAC模型下的Mg2+(1s-2)退激发后不产生6价离子.Based on the conclusion that the contribution of correlated decay of two vacancies in atoms is small, the de-excitation process of Mg^1+ (ls^-1) hollow magnesium ions with single K-vacancy and Mg^2+ (ls^-2) double K-vacancy were treated by applying the radiative-single Auger - double Auger cascade model(RACDA). The final-charge-state distribution(FCSD) of these hollow ions were calculated, and compared with that obtained with the radiative-single Auger cascade model(RAC). The probability of tetravalent ion production via the de-excitation of Mg^1+ (1 s^-1 ) obtained by RACDA model is considerable, but tetravalent ion is not produced in the by RAC model. The probability of hexavalent ion production via the de-excitation of Mg^2+ ( 1 s^- 2 ) obtained by RACDA model is very large, but hexavalent ion is not produced in the RAC model.
关 键 词:双洞态退激发 RACDA退激发模型 末电离态离子分布
分 类 号:O562.1[理学—原子与分子物理]
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