Characterization of specific nuclear reaction channels by deconvolution in the energy space of the total nuclear cross-section of protons - applications to proton therapy and technical problems (transmutations)

W. Ulmer
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引用次数: 2

Abstract

The total nuclear cross-section Qtot(E) resulting from the interaction of protons with nuclei is decomposed in 3 different contributions: 1. elastic scatter at the complete nucleus, which adopts a part of the proton kinetic energy; 2. inelastic scatter at a nucleus, which changes its quantum numbers by vibrations, rotations, transition to highly excited states; 3. proper nuclear reactions with change of the mass and/or charge number. Then different particles leave the hit nucleus (neutrons, protons, etc.), which is now referred to as 'heavy recoil' nucleus. The scatter parts of Qtot(E) according to points 1 and 2 can be removed by a deconvolution acting at Qtot(E) in the energy space. The typical nuclear reaction channels are mainly characterized by resonances of a reduced cross-section function Qred(E). The procedure is applied to cross-sections of therapeutic protons and also to Cs55137 as an example with technical relevance (transmutations with the goal to drastically reduce its half-time).
通过质子总核截面能量空间的反褶积来表征特定核反应通道。在质子治疗和技术问题(嬗变)中的应用
由质子与原子核相互作用产生的总核截面Qtot(E)分解为三个不同的贡献:1。弹性散射在完整的原子核处,吸收了一部分质子的动能;2. 原子核上的非弹性散射,通过振动、旋转、跃迁到高激发态来改变其量子数;3.随质量和/或电荷数变化的适当核反应。然后,不同的粒子离开被击中的核(中子、质子等),现在被称为“重反冲”核。Qtot(E)根据点1和2的散射部分可以通过能量空间中作用于Qtot(E)的反褶积去除。典型的核反应通道主要以截面函数Qred(E)的共振为特征。该程序应用于治疗性质子的横截面,也应用于Cs55137作为一个具有技术相关性的例子(以大幅度减少其半截时间为目标的嬗变)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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