首页> 外文期刊>Instruments and Experimental Techniques >A Method for Determining the Intensity of Concomitant Neutron Source D(d, n)3{sup left}He when Studying the Characteristics of Delayed Neutrons from Nuclear Fission Induced by Neutrons from Reaction T(d, n)4{sup left}He
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A Method for Determining the Intensity of Concomitant Neutron Source D(d, n)3{sup left}He when Studying the Characteristics of Delayed Neutrons from Nuclear Fission Induced by Neutrons from Reaction T(d, n)4{sup left}He

机译:研究反应T(d,n)4 {{}}}的中子引起的核裂变延迟中子的特性时,确定伴随中子源D(d,n)3 {He}的强度的方法

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摘要

A factor that may be responsible for the discrepancies in the total delay neutron yields, the relative yields of separate groups of delayed neutrons, and half-lives of their precursors has been investigated. These discrepancies are shown to be attributable to the effect of a concomitant neutron source - reaction D(d, n)3{sup left}He. Such a source is unavoidably present in an experiment where reaction T(d, n)4He on a solid-state target is used as a neutron source. A method has been developed to calculate the contribution of neutrons from the reaction D(d, n)3{sup left}He to the measured total and relative yields of delayed neutrons and the half-lives of their precursors in heavy nuclei fission induced by neutrons with energies of 14-18 MeV. The energy dependence of the parameters of delayed neutron groups from the neutron-induced fission of 238{sup left}U nuclei in the energy range of 14.2-17.9 MeV is presented.
机译:已经研究了可能导致总延迟中子产率差异,延迟中子的单独组的相对产率以及其前体半衰期差异的因素。这些差异被证明归因于伴随的中子源的作用-反应D(d,n)3 {sup left} He。这种源不可避免地存在于将固态靶上的反应T(d,n)4He用作中子源的实验中。已经开发了一种方法来计算反应D(d,n)3 {中} He对中子的贡献,该中子对测得的迟发中子的总和相对产率以及由中子诱发的重核裂变中它们的前体的半衰期的半衰期能量为14-18 MeV的中子。提出了由中子引起的238 {U核裂变的中子群延迟参数的能量依赖性,其能量范围为14.2-17.9 MeV。

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