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双核系统核子转移驱动势与复合核的最佳激发能
引用本文:李剑锋,徐瑚珊,李文飞,左维,李君清,王楠,赵恩广.双核系统核子转移驱动势与复合核的最佳激发能[J].原子核物理评论,2003,20(2):160-164.
作者姓名:李剑锋  徐瑚珊  李文飞  左维  李君清  王楠  赵恩广
作者单位:1 中国科学院近代物理研究所; 甘肃兰州; 730000; 2 兰州重离子加速器国家实验室原子核理论中心 甘肃兰州 730000;3 中国科学院理论物理研究所; ; 北京100080;
基金项目:国家自然科学基金资助项目(10175082),中国科学院知识创新工程重点方向性资助项目(KJCX2 N11),中国科学院百人计划资助项目,国家重点研究发展规划资助项目(G2000077400),科技部基础研究重大项目前期研究专项基金资助项目
摘    要:计算了以208Pb为靶的一系列重离子熔合反应双核系统核子转移驱动势.它制约由输运方程所支配的核子转移速率,因而确定了双核系统形成复合核的几率.并由此可确定形成复合核所必须的最低激发能,即形成最稳定复合核的最佳激发能,得到了与已知实验值基本符合的结果. Particle transfer driven potentials in Di nuclear System (DNS) in heavy ion collisions based on 208Pb target are calculated. The driven potential controls the particle transfer velocity in the process governed by the diffusion equation, and as a consequence determines the compound nuclear formation probability of DNS. The minimum excitation energy to form a compound nucleus, which is the optimum excitation energy to form the most stable compound nucleus, has been calculated, and the results are basica...

关 键 词:超重核    驱动势    全熔合    准裂变    最佳激发能
文章编号:1007-4627(2003)02-0160-05
收稿时间:1900-01-01
修稿时间:2003年1月25日

Nucleon Transfer Driven Potential and the Optimum Excitation Energy of Compound Nucleus Formed in Dinuclear Systems
Institution:(1 Institute of Modern Physics; Chinese Academy of Sciences; Lanzhou 730000; China;2 Center of Theoretical Nuclear Physics; National Laboratory of Heavy Ion Accelerator of Lanzhou; 3 Institute of Theoretical Physics; Beijing 100080; China);
Abstract:Particle transfer driven potentials in Di nuclear System (DNS) in heavy ion collisions based on 208Pb target are calculated. The driven potential controls the particle transfer velocity in the process governed by the diffusion equation, and as a consequence determines the compound nuclear formation probability of DNS. The minimum excitation energy to form a compound nucleus, which is the optimum excitation energy to form the most stable compound nucleus, has been calculated, and the results are basica...
Keywords:super-heavy nucleus  driven potential  complete fusion  quasifission  optimum excitation energy
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