Angular and energy distribution of fission neutrons

G.A. Bat, L.P. Kudrin
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引用次数: 2

Abstract

The angular distribution of fission neutrons given by the statistical model of the nucleus is calculated, taking account of the angular anisotropy of emission of fission fragments. The latter is represented by the simple expression 1 + k cos2α. It is assumed that the neutrons are emitted isotropically in the co-ordinate system in which the appropriate fragment is at rest. The ratio P of fission neutron intensities emitted parallel and perpendicular to the primary neutron beam is calculated for 238U, the energy range 1–10 MeV being covered for both primary and secondary neutrons. When the fission is considered to be induced by neutrons of the fission spectrum, the mean value of P for 238U comes to ∼1·13. The energy spectrum of the fission neutrons is also calculated for various values of the incident neutron energy. Anisotropies occurring in the fission of other nuclei may be calculated by the same method.

裂变中子的角分布和能量分布
考虑到裂变碎片发射的角各向异性,计算了核统计模型给出的裂变中子的角分布。后者由简单的表达式1 + k cos2α表示。假定中子在相应的碎片静止的坐标系中是各向同性发射的。计算了238U时平行和垂直于主中子束发射的裂变中子强度的比值P,其中主中子和次级中子的能量范围均为1-10 MeV。当认为裂变是由裂变谱中的中子引起时,238U的P平均值为~ 1·13。根据入射中子能量的不同值,还计算了裂变中子的能谱。发生在其他原子核裂变中的各向异性可以用同样的方法来计算。
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