{"title":"242mAm衰变的分支比","authors":"R.W. Hoff, E.K. Hulet, M.C. Michel","doi":"10.1016/0891-3919(59)90006-3","DOIUrl":null,"url":null,"abstract":"<div><p>The branching ratio, <em>β</em><sup>−</sup>/<em>EC</em> = 5·1 ± 0·1, for <sup>242<em>m</em></sup>Am decay has been measured by determining the relative amounts of the decay products, <sup>242</sup>Cm and <sup>242</sup>Pu formed. The 16 hour <sup>242<em>m</em></sup>Am was produced by neutron irradiation of <sup>241</sup>Am in the Materials Testing Reactor. A pile neutron cross-section of 620 ± 65 barns for the reaction <sup>241</sup>Am(n, γ)<sup>242m</sup>Am was measured.</p></div>","PeriodicalId":100812,"journal":{"name":"Journal of Nuclear Energy (1954)","volume":"8 4","pages":"Pages 224-228"},"PeriodicalIF":0.0000,"publicationDate":"1959-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0891-3919(59)90006-3","citationCount":"9","resultStr":"{\"title\":\"Branching ratio of 242mAm decay\",\"authors\":\"R.W. Hoff, E.K. Hulet, M.C. Michel\",\"doi\":\"10.1016/0891-3919(59)90006-3\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The branching ratio, <em>β</em><sup>−</sup>/<em>EC</em> = 5·1 ± 0·1, for <sup>242<em>m</em></sup>Am decay has been measured by determining the relative amounts of the decay products, <sup>242</sup>Cm and <sup>242</sup>Pu formed. The 16 hour <sup>242<em>m</em></sup>Am was produced by neutron irradiation of <sup>241</sup>Am in the Materials Testing Reactor. A pile neutron cross-section of 620 ± 65 barns for the reaction <sup>241</sup>Am(n, γ)<sup>242m</sup>Am was measured.</p></div>\",\"PeriodicalId\":100812,\"journal\":{\"name\":\"Journal of Nuclear Energy (1954)\",\"volume\":\"8 4\",\"pages\":\"Pages 224-228\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1959-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0891-3919(59)90006-3\",\"citationCount\":\"9\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Nuclear Energy (1954)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0891391959900063\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Nuclear Energy (1954)","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0891391959900063","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The branching ratio, β−/EC = 5·1 ± 0·1, for 242mAm decay has been measured by determining the relative amounts of the decay products, 242Cm and 242Pu formed. The 16 hour 242mAm was produced by neutron irradiation of 241Am in the Materials Testing Reactor. A pile neutron cross-section of 620 ± 65 barns for the reaction 241Am(n, γ)242mAm was measured.