Review and Evaluation of the Spontaneous Fission Half-lives of 238Pu, 240Pu, and 242Pu and the Corresponding Specific Fission Rates

IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Nuclear Data Sheets Pub Date : 2021-07-01 DOI:10.1016/j.nds.2021.06.003
Stephen Croft , Andrea Favalli
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引用次数: 2

Abstract

A widely applied technical measure of nuclear safeguards and nonproliferation for the nondestructive verification and mass-assay of items containing separated plutonium is passive neutron multiplicity counting. The primary source of time correlated passive neutrons is the spontaneous fission of Pu, where the 240Pu is usually the dominant isotope with 238Pu and 242Pu also contributing to a degree depending on the grade or burnup of the material. Consequently, knowledge of the 240Pu spontaneous fission rate, expressed as fission per gram per second, and the associated uncertainty is key in interpreting measurement data absolutely. The 240Pu spontaneous fission rate derives (and vice versa) from the 240Pu spontaneous fission half-life. In this work we review and reevaluate the available experimental data on the spontaneous fission (SF) half-life of the Pu isotopes 238Pu, 240Pu and 242Pu. The SF half-lives are used to compute the corresponding specific SF rates which are the traditional nuclear data parameters needed for analytical applications, especially the nondestructive assay of plutonium for safety, security and safeguards.

From 7 measurements we recommend a SF half-life of (4.745 ± 0.083) × 1010 y for 238Pu corresponding to a specific SF rate of (1171 ± 20) fis ⋅ s-1 ⋅ g-1.

There are 16 absolute experimental determinations of 240Pu half-life. Based on this evaluation, we find that the weighted mean of the 16 half-life determinations is (1.1608 ± 0.0091) × 1011 y corresponding to a specific SF rate of (474.7 ± 3.7) fis ⋅ s−1 ⋅ g−1, where the relative uncertainty of about 0.78% is the external standard error.

From 8 measurements we recommend a SF half-life of (6.766 ± 0.037) × 1010 y for 242Pu corresponding to a specific SF rate of (807.7 ± 4.4) fis ⋅ s−1 ⋅ g−1. Finally, we conclude that there is a need for more experiments on all three plutonium nuclides using new techniques that have emerged in recent years.

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238Pu、240Pu和242Pu的自发裂变半衰期及相应的比裂变率的回顾与评价
被动中子多重计数是一种广泛应用于核保障和核不扩散的技术措施,用于对含有分离钚的物项进行无损核查和质量分析。时间相关被动中子的主要来源是Pu的自发裂变,其中240Pu通常是主要同位素,238Pu和242Pu也有一定程度的贡献,这取决于材料的等级或燃燃量。因此,了解240Pu的自发裂变率(表示为每克每秒裂变)以及相关的不确定度是绝对解释测量数据的关键。240Pu的自发裂变速率来源于(反之亦然)240Pu的自发裂变半衰期。本文对铀同位素238Pu、240Pu和242Pu的自发裂变(SF)半衰期的实验数据进行了回顾和重新评价。SF半衰期用于计算相应的特定SF速率,这是传统的核数据参数,用于分析应用,特别是用于安全,安保和保障的钚的无损分析。从7次测量中,我们推荐238Pu的SF半衰期为(4.745±0.083)× 1010 y,对应的特定SF率为(1171±20)fis⋅s-1⋅g-1。240Pu的半衰期有16个绝对实验测定。基于此评价,我们发现16个半衰期测定的加权平均值为(1.1608±0.0091)× 1011 y,对应的特定SF率为(474.7±3.7)fis⋅s−1⋅g−1,其中相对不确定度约为0.78%为外部标准误差。从8次测量中,我们推荐242Pu的SF半衰期为(6.766±0.037)× 1010 y,对应的特定SF率为(807.7±4.4)fis⋅s−1⋅g−1。最后,我们的结论是,有必要利用近年来出现的新技术对所有三种钚核素进行更多的实验。
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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来源期刊
Nuclear Data Sheets
Nuclear Data Sheets 物理-物理:核物理
CiteScore
7.80
自引率
5.40%
发文量
22
审稿时长
>12 weeks
期刊介绍: The Nuclear Data Sheets are current and are published monthly. They are devoted to compilation and evaluations of experimental and theoretical results in Nuclear Physics. The journal is mostly produced from Evaluated Nuclear Structure Data File (ENSDF), a computer file maintained by the US National Nuclear Data Center
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