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Nonuniform character of the population of spin projections K for a fissile nucleus at the scission point and anisotropies in the angular distributions of fragments originating from the induced fission of nuclei

机译:裂变原子核在分裂点的自旋投影K种群的不均匀特征以及由诱导核裂变产生的碎片的角度分布的各向异性

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摘要

It is shown that the emergence of anisotropies in the angular distributions of fragments originating from the spontaneous and induced fission of oriented actinide nuclei is possible only if nonuniformities in the population of the projectionsM (K) of the fissile-nucleus spin onto the z axis of the laboratory frame (fissile-nucleus symmetry axis) appear simultaneously in the vicinity of the scission point but not in the vicinity of the outer saddle point of the deformation potential. The possibilities for creating the orientation of fissile nuclei for spontaneous and induced fission and the effect of these orientations on the anisotropies under analysis are considered. The role of Coriolis interaction as a unique source of the mixing of different-K fissile-nucleus states at all stages of the fission process is studied with allowance for the dynamical enhancement of this interaction for excited thermalized states of the nucleus involved that is characterized by a high energy density. It is shown that the absence of thermalization of excited states of the fissile nucleus that appear because of the effect of nonadiabaticity of its collective deformation motion in the vicinity of the scission point is a condition of conservation of the influence that transition fission states formed at the inner and outer fission barriers exerts on the distribution of the spin projections K for lowenergy spontaneous nuclear fission. It is confirmed that anisotropies observed in the angular distributions of fragments originating from the fission of nuclei that is induced by fast light particles (multiply charged ions) are due to the appearance of strongly excited equilibrium(nonequilibrium) states of the fissile nucleus in the vicinity of its scission point that have a Gibbs (non-Gibbs) distribution of projections K.
机译:结果表明,只有当易裂变核的投影M(K)的总体不均匀旋转到Z轴的z轴上时,取向oriented系原子的自发和诱导裂变所产生的碎片的角分布中才会出现各向异性。实验室框架(裂变核对称轴)同时出现在断裂点附近,而不出现在变形势的外鞍点附近。考虑了为自发裂变和诱发裂变创建裂变核取向的可能性,以及这些取向对所分析各向异性的影响。研究了科里奥利相互作用作为裂变过程各个阶段中不同K裂变核态混合的唯一来源的作用,并允许动态增强所涉及核的激发热态的相互作用,其特征在于高能量密度。结果表明,在裂变点附近,由于其集体变形运动的非绝热性而引起的裂变核激发态的热化不存在,是保持在裂变点处形成的过渡裂变态的影响的条件。内部和外部裂变壁垒作用在自旋突起K的分布上,以实现低能自发核裂变。可以确定的是,在快光粒子(带多个电荷的离子)引起的原子核裂变所产生的碎片的角分布中观察到的各向异性是由于在附近出现了裂变核的强烈激发的平衡态(非平衡态)的分裂点具有投影K的吉布斯(非吉布斯)分布。

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