计算物理 ›› 2022, Vol. 39 ›› Issue (6): 631-640.DOI: 10.19596/j.cnki.1001-246x.8539
• 研究论文 • 下一篇
收稿日期:
2022-03-30
出版日期:
2022-11-25
发布日期:
2023-04-01
通讯作者:
叶涛
作者简介:
周历波, 男, 硕士研究生, 研究方向为粒子物理与原子核物理, E-mail: zhoulibo19@gscaep.ac.cn
Libo ZHOU1(), Tao YE2,*(
), Jia WANG2, Weili SUN2
Received:
2022-03-30
Online:
2022-11-25
Published:
2023-04-01
Contact:
Tao YE
摘要:
以广义约化R矩阵理论为基础, 运用RAC程序(R-matrix analysis code)综合分析有关4He系统的所有核反应的实验数据, 给出从0~30 MeV范围内一套完整的评价值, 各反应数据内部自恰。其中积分截面的拟合包括3He(n, total)、3He(n, n)3He、3He(n, d)D、3He(n, p)T、D(d, n)3He、D(d, p)T和T(p, n)3He, 同时给出相应的误差矩阵; 天体物理学S因子的拟合包括D(d, n)3He和D(d, p)T; 微分截面的拟合包括3He(n, n)3He、3He(n, p)T、D(d, d)D、D(d, n)3He和D(d, p)T。所有的拟合结果与实验数据和主流评价数据符合良好。在低能部分, 提高了D(d, n)3He反应和D(d, p)T反应各自积分截面的精确度。在高能部分, 将4He系统的评价数据进行了扩展。
周历波, 叶涛, 王佳, 孙伟力. 4He系统的广义约化R矩阵理论分析[J]. 计算物理, 2022, 39(6): 631-640.
Libo ZHOU, Tao YE, Jia WANG, Weili SUN. A Theoretical Analysis of Generalized Reduced R-Matrix of 4He System[J]. Chinese Journal of Computational Physics, 2022, 39(6): 631-640.
Reaction channel | Radius ac/fm | Threshold/MeV |
3He + n | 3.530 0 | 0 |
D + d | 5.956 3 | -3.268 9 |
T + p | 5.485 9 | 0.763 8 |
D + np | 6.825 0 | -5.493 4 |
P + 2np | 6.825 0 | -7.717 9 |
表1 反应道的道半径和阈值
Table 1 Radius and threshold of reaction channels
Reaction channel | Radius ac/fm | Threshold/MeV |
3He + n | 3.530 0 | 0 |
D + d | 5.956 3 | -3.268 9 |
T + p | 5.485 9 | 0.763 8 |
D + np | 6.825 0 | -5.493 4 |
P + 2np | 6.825 0 | -7.717 9 |
Reaction | Cross section type | Incident energy region/MeV | Number of data points | Relative error of LOWESS results/% |
3He(n, tot) | Total | 1×10-11 to 40 | 1639 | 1.9 |
3He(n, n)3He | Integral | 1×10-11 to 30 | 147 | 1.9 |
3He(n, p)3He | Integral | 1×10-10 to 30 | 237 | 4.5 |
3He(n, d)3He | Integral | 4.36 to 30 | 58 | 9 |
D(d, p)T | Integral | 0.014 5 to 38.5 | 78 | 1.2 |
D(d, n)3He | Integral | 0.006 8 to 38.5 | 169 | 1.6 |
3He(n, np)D | Integral | 7.9 to 23.7 | 5 | |
3He(n, 2np)P | Integral | 14 to 30 | 8 | |
T(p, n)3He | Integral | 0.35 to 14.44 | 397 | 4 |
D(d, d)D | Differential | 0.96 to 13.45 | 1 038 | |
D(d, n)3He | Differential | 0.019 94 to 18 | 437 | |
D(d, p)T | Differential | 0.019 94 to 13.2 | 967 | |
3He(n, d)D | Differential | 14.4 | 12 | |
3He(n, n)3He | Differential | 1 to 30 | 396 | |
3He(n, p)T | Differential | 0.01 to 14.44 | 294 | |
T(p, p)T | Differential | 0.35 to 16.34 | 478 | |
Total | 1×10-11 to 40 | 6 360 |
表2 实验数据的使用和光滑处理的相对误差
Table 2 The usage of experimental data and relative error of smoothing
Reaction | Cross section type | Incident energy region/MeV | Number of data points | Relative error of LOWESS results/% |
3He(n, tot) | Total | 1×10-11 to 40 | 1639 | 1.9 |
3He(n, n)3He | Integral | 1×10-11 to 30 | 147 | 1.9 |
3He(n, p)3He | Integral | 1×10-10 to 30 | 237 | 4.5 |
3He(n, d)3He | Integral | 4.36 to 30 | 58 | 9 |
D(d, p)T | Integral | 0.014 5 to 38.5 | 78 | 1.2 |
D(d, n)3He | Integral | 0.006 8 to 38.5 | 169 | 1.6 |
3He(n, np)D | Integral | 7.9 to 23.7 | 5 | |
3He(n, 2np)P | Integral | 14 to 30 | 8 | |
T(p, n)3He | Integral | 0.35 to 14.44 | 397 | 4 |
D(d, d)D | Differential | 0.96 to 13.45 | 1 038 | |
D(d, n)3He | Differential | 0.019 94 to 18 | 437 | |
D(d, p)T | Differential | 0.019 94 to 13.2 | 967 | |
3He(n, d)D | Differential | 14.4 | 12 | |
3He(n, n)3He | Differential | 1 to 30 | 396 | |
3He(n, p)T | Differential | 0.01 to 14.44 | 294 | |
T(p, p)T | Differential | 0.35 to 16.34 | 478 | |
Total | 1×10-11 to 40 | 6 360 |
图11 3He(n, n)3He弹性散射微分截面(部分),入射能分别为(a) =6 MeV;(b) =14.4 MeV;(c)16 MeV;(d)27 MeV
Fig.11 Differential cross sections of 3He(n, n)3He (partial) at incident energies (a)6 MeV; (b)14.4 MeV; (c)16 MeV; (d)27 MeV
图12 D(d, d)D弹性散射微分截面(部分),入射能分别为(a)0.96 MeV;(b)2.51 MeV;(c)10.5 MeV;(d)13.2 MeV
Fig.12 Differential cross sections of D(d, d)D (partial) at incident energies (a)0.96 MeV; (b)2.51 MeV; (c)10.5 MeV; (d)13.2 MeV
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