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(n,p)和(n,α)激发函数半经验计算方法

樊胜 阎芳 张鸿洲 赵志祥

樊胜, 阎芳, 张鸿洲, 赵志祥. (n,p)和(n,α)激发函数半经验计算方法[J]. 原子核物理评论, 2004, 21(4): 389-390. doi: 10.11804/NuclPhysRev.21.04.389
引用本文: 樊胜, 阎芳, 张鸿洲, 赵志祥. (n,p)和(n,α)激发函数半经验计算方法[J]. 原子核物理评论, 2004, 21(4): 389-390. doi: 10.11804/NuclPhysRev.21.04.389
FAN Sheng, YAN Yang, ZHANG Hong-zhou, ZHAO Zhi-xiang. Semi-empirical Method for (n, p) and (n, α) Reactions Excitation Function[J]. Nuclear Physics Review, 2004, 21(4): 389-390. doi: 10.11804/NuclPhysRev.21.04.389
Citation: FAN Sheng, YAN Yang, ZHANG Hong-zhou, ZHAO Zhi-xiang. Semi-empirical Method for (n, p) and (n, α) Reactions Excitation Function[J]. Nuclear Physics Review, 2004, 21(4): 389-390. doi: 10.11804/NuclPhysRev.21.04.389

(n,p)和(n,α)激发函数半经验计算方法

doi: 10.11804/NuclPhysRev.21.04.389

Semi-empirical Method for (n, p) and (n, α) Reactions Excitation Function

  • 摘要: 在En≤20MeV的情况下,忽略了粒子的二次发射过程,认为复合系统的形成截面是能量相关的,得到了理论模型清晰、公式形式简单的半经验计算方法.在靶核23≤A≤209的范围内,利用大量(n,p)和(n,α)反应的截面实验数据对可调参数进行了研究,得到了参数对靶核的N和Z以及入射能量的依赖关系.对得到的参数做了定性的解释,利用普适参数对(n,p)和(n,α)反应的激发函数做了预言,预言值在其误差范围内与实验数据一致. To simplify the calculation, some assumptions are considered at present work. The preequilibrium emission is the first step in the equilibrium process, which is characterized by exciton n=3 and "never come back" are considered at the preequilibrium emission process; the proton and alpha emissions are only competed with the neutron emission, the second particle emission is neglected. A semiempirical method of the cross section for (n, p ) and (n, α) reactions were obtained on the basis of evaporatio...
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出版历程
  • 收稿日期:  1900-01-01
  • 修回日期:  1900-01-01
  • 刊出日期:  2004-12-20

(n,p)和(n,α)激发函数半经验计算方法

doi: 10.11804/NuclPhysRev.21.04.389

摘要: 在En≤20MeV的情况下,忽略了粒子的二次发射过程,认为复合系统的形成截面是能量相关的,得到了理论模型清晰、公式形式简单的半经验计算方法.在靶核23≤A≤209的范围内,利用大量(n,p)和(n,α)反应的截面实验数据对可调参数进行了研究,得到了参数对靶核的N和Z以及入射能量的依赖关系.对得到的参数做了定性的解释,利用普适参数对(n,p)和(n,α)反应的激发函数做了预言,预言值在其误差范围内与实验数据一致. To simplify the calculation, some assumptions are considered at present work. The preequilibrium emission is the first step in the equilibrium process, which is characterized by exciton n=3 and "never come back" are considered at the preequilibrium emission process; the proton and alpha emissions are only competed with the neutron emission, the second particle emission is neglected. A semiempirical method of the cross section for (n, p ) and (n, α) reactions were obtained on the basis of evaporatio...

English Abstract

樊胜, 阎芳, 张鸿洲, 赵志祥. (n,p)和(n,α)激发函数半经验计算方法[J]. 原子核物理评论, 2004, 21(4): 389-390. doi: 10.11804/NuclPhysRev.21.04.389
引用本文: 樊胜, 阎芳, 张鸿洲, 赵志祥. (n,p)和(n,α)激发函数半经验计算方法[J]. 原子核物理评论, 2004, 21(4): 389-390. doi: 10.11804/NuclPhysRev.21.04.389
FAN Sheng, YAN Yang, ZHANG Hong-zhou, ZHAO Zhi-xiang. Semi-empirical Method for (n, p) and (n, α) Reactions Excitation Function[J]. Nuclear Physics Review, 2004, 21(4): 389-390. doi: 10.11804/NuclPhysRev.21.04.389
Citation: FAN Sheng, YAN Yang, ZHANG Hong-zhou, ZHAO Zhi-xiang. Semi-empirical Method for (n, p) and (n, α) Reactions Excitation Function[J]. Nuclear Physics Review, 2004, 21(4): 389-390. doi: 10.11804/NuclPhysRev.21.04.389

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