G. Satyanarayana, V. Ramamurty, V. Lakshminarayana
{"title":"321 keV(9/2-)状态在125Te下的寿命","authors":"G. Satyanarayana, V. Ramamurty, V. Lakshminarayana","doi":"10.1088/0305-4470/5/8/017","DOIUrl":null,"url":null,"abstract":"The halflife of the 321 keV(9/2-) state in 125Te is measured by the delayed coincidence technique employing a time-to-amplitude converter. On comparing the experimental M1 and E2 transition probabilities with those evaluated by the single particle model, Kisslinger's three-quasiparticle model and the De-Shalit model, it is found that De-Shalit's single particle-core coupling model is applicable in this case.","PeriodicalId":54612,"journal":{"name":"Physics-A Journal of General and Applied Physics","volume":"31 1","pages":"1243-1247"},"PeriodicalIF":0.0000,"publicationDate":"1972-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Lifetime of the 321 keV(9/2-) state in 125Te\",\"authors\":\"G. Satyanarayana, V. Ramamurty, V. Lakshminarayana\",\"doi\":\"10.1088/0305-4470/5/8/017\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The halflife of the 321 keV(9/2-) state in 125Te is measured by the delayed coincidence technique employing a time-to-amplitude converter. On comparing the experimental M1 and E2 transition probabilities with those evaluated by the single particle model, Kisslinger's three-quasiparticle model and the De-Shalit model, it is found that De-Shalit's single particle-core coupling model is applicable in this case.\",\"PeriodicalId\":54612,\"journal\":{\"name\":\"Physics-A Journal of General and Applied Physics\",\"volume\":\"31 1\",\"pages\":\"1243-1247\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1972-08-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physics-A Journal of General and Applied Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1088/0305-4470/5/8/017\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physics-A Journal of General and Applied Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/0305-4470/5/8/017","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The halflife of the 321 keV(9/2-) state in 125Te is measured by the delayed coincidence technique employing a time-to-amplitude converter. On comparing the experimental M1 and E2 transition probabilities with those evaluated by the single particle model, Kisslinger's three-quasiparticle model and the De-Shalit model, it is found that De-Shalit's single particle-core coupling model is applicable in this case.
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