{"title":"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","authors":"Stephen Croft , Andrea Favalli","doi":"10.1016/j.nds.2021.06.003","DOIUrl":null,"url":null,"abstract":"<div><p>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 <sup>240</sup>Pu is usually the dominant isotope with <sup>238</sup>Pu and <sup>242</sup>Pu also contributing to a degree depending on the grade or burnup of the material. Consequently, knowledge of the <sup>240</sup>Pu spontaneous fission rate, expressed as fission per gram per second, and the associated uncertainty is key in interpreting measurement data absolutely. The <sup>240</sup>Pu spontaneous fission rate derives (and vice versa) from the <sup>240</sup>Pu 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 <sup>238</sup>Pu, <sup>240</sup>Pu and <sup>242</sup>Pu. 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.</p><p>From 7 measurements we recommend a SF half-life of (4.745 ± 0.083) × 10<sup>10</sup> <em>y</em> for <sup>238</sup>Pu corresponding to a specific SF rate of (1171 ± 20) fis ⋅ s<sup>-1</sup> ⋅ g<sup>-1</sup>.</p><p>There are 16 absolute experimental determinations of <sup>240</sup>Pu half-life. Based on this evaluation, we find that the weighted mean of the 16 half-life determinations is (1.1608 ± 0.0091) × 10<sup>11</sup> <em>y</em> corresponding to a specific SF rate of (474.7 ± 3.7) fis ⋅ s<sup>−1</sup> ⋅ g<sup>−1</sup>, where the relative uncertainty of about 0.78% is the external standard error.</p><p>From 8 measurements we recommend a SF half-life of (6.766 ± 0.037) × 10<sup>10</sup> <em>y</em> for <sup>242</sup>Pu corresponding to a specific SF rate of (807.7 ± 4.4) fis ⋅ s<sup>−1</sup> ⋅ g<sup>−1</sup>. 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.</p></div>","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"175 ","pages":"Pages 269-287"},"PeriodicalIF":2.8000,"publicationDate":"2021-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/j.nds.2021.06.003","citationCount":"2","resultStr":"{\"title\":\"Review and Evaluation of the Spontaneous Fission Half-lives of 238Pu, 240Pu, and 242Pu and the Corresponding Specific Fission Rates\",\"authors\":\"Stephen Croft , Andrea Favalli\",\"doi\":\"10.1016/j.nds.2021.06.003\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>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 <sup>240</sup>Pu is usually the dominant isotope with <sup>238</sup>Pu and <sup>242</sup>Pu also contributing to a degree depending on the grade or burnup of the material. Consequently, knowledge of the <sup>240</sup>Pu spontaneous fission rate, expressed as fission per gram per second, and the associated uncertainty is key in interpreting measurement data absolutely. The <sup>240</sup>Pu spontaneous fission rate derives (and vice versa) from the <sup>240</sup>Pu 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 <sup>238</sup>Pu, <sup>240</sup>Pu and <sup>242</sup>Pu. 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.</p><p>From 7 measurements we recommend a SF half-life of (4.745 ± 0.083) × 10<sup>10</sup> <em>y</em> for <sup>238</sup>Pu corresponding to a specific SF rate of (1171 ± 20) fis ⋅ s<sup>-1</sup> ⋅ g<sup>-1</sup>.</p><p>There are 16 absolute experimental determinations of <sup>240</sup>Pu half-life. Based on this evaluation, we find that the weighted mean of the 16 half-life determinations is (1.1608 ± 0.0091) × 10<sup>11</sup> <em>y</em> corresponding to a specific SF rate of (474.7 ± 3.7) fis ⋅ s<sup>−1</sup> ⋅ g<sup>−1</sup>, where the relative uncertainty of about 0.78% is the external standard error.</p><p>From 8 measurements we recommend a SF half-life of (6.766 ± 0.037) × 10<sup>10</sup> <em>y</em> for <sup>242</sup>Pu corresponding to a specific SF rate of (807.7 ± 4.4) fis ⋅ s<sup>−1</sup> ⋅ g<sup>−1</sup>. 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.</p></div>\",\"PeriodicalId\":49735,\"journal\":{\"name\":\"Nuclear Data Sheets\",\"volume\":\"175 \",\"pages\":\"Pages 269-287\"},\"PeriodicalIF\":2.8000,\"publicationDate\":\"2021-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/j.nds.2021.06.003\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Data Sheets\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0090375221000363\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Data Sheets","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0090375221000363","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, NUCLEAR","Score":null,"Total":0}
Review and Evaluation of the Spontaneous Fission Half-lives of 238Pu, 240Pu, and 242Pu and the Corresponding Specific Fission Rates
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) × 1010y 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) × 1011y 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) × 1010y 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.
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