{"title":"利用宏观-微观方法中的卡西尼椭圆参数化研究 $$^{236}$ U 和 $$^{233}$ Th 的静态裂变特性","authors":"P. Jachimowicz, R. Capote, M. Kowal","doi":"10.1140/epja/s10050-024-01381-9","DOIUrl":null,"url":null,"abstract":"<div><p>We have conducted a thorough analysis of the potential energy surfaces (PES) in <span>\\(^{236}\\)</span>U and <span>\\(^{233}\\)</span>Th using the Cassini-ovals parameterization within the macro–micro approach. We employed the state-of-the-art immersion water flow (IWF) method to study the saddles on four-dimensional energy grids encompassing reflection-asymmetric shapes. For <span>\\(^{233}\\)</span>Th, we computed the adiabatic potential energy surfaces by minimizing configurations with one blocked neutron within ten levels below and above the Fermi level. Our results show satisfactory agreement with empirical and experimental estimates for both nuclei, specifically regarding the first and second fission barriers. This suggests that our method holds promise in efficiently describing non-compact shapes while reducing the dimensionality of the space without sacrificing accuracy. Interestingly, employing Cassinian oval parameterization fails to reveal a pronounced, hyper-deformed third minimum in the potential energy landscape. Instead, only a shallow third minimum is observed for <span>\\(^{233}\\)</span>Th, while in <span>\\(^{236}\\)</span>U, this minimum ultimately vanishes. This finding holds significant importance when considering the modeling of fission cross-sections.</p></div>","PeriodicalId":786,"journal":{"name":"The European Physical Journal A","volume":"60 8","pages":""},"PeriodicalIF":2.6000,"publicationDate":"2024-08-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epja/s10050-024-01381-9.pdf","citationCount":"0","resultStr":"{\"title\":\"Examination of static fission properties of \\\\(^{236}\\\\)U and \\\\(^{233}\\\\)Th using Cassinian oval parametrization within the macroscopic–microscopic approach\",\"authors\":\"P. Jachimowicz, R. Capote, M. Kowal\",\"doi\":\"10.1140/epja/s10050-024-01381-9\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We have conducted a thorough analysis of the potential energy surfaces (PES) in <span>\\\\(^{236}\\\\)</span>U and <span>\\\\(^{233}\\\\)</span>Th using the Cassini-ovals parameterization within the macro–micro approach. We employed the state-of-the-art immersion water flow (IWF) method to study the saddles on four-dimensional energy grids encompassing reflection-asymmetric shapes. For <span>\\\\(^{233}\\\\)</span>Th, we computed the adiabatic potential energy surfaces by minimizing configurations with one blocked neutron within ten levels below and above the Fermi level. Our results show satisfactory agreement with empirical and experimental estimates for both nuclei, specifically regarding the first and second fission barriers. This suggests that our method holds promise in efficiently describing non-compact shapes while reducing the dimensionality of the space without sacrificing accuracy. Interestingly, employing Cassinian oval parameterization fails to reveal a pronounced, hyper-deformed third minimum in the potential energy landscape. Instead, only a shallow third minimum is observed for <span>\\\\(^{233}\\\\)</span>Th, while in <span>\\\\(^{236}\\\\)</span>U, this minimum ultimately vanishes. This finding holds significant importance when considering the modeling of fission cross-sections.</p></div>\",\"PeriodicalId\":786,\"journal\":{\"name\":\"The European Physical Journal A\",\"volume\":\"60 8\",\"pages\":\"\"},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2024-08-02\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1140/epja/s10050-024-01381-9.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The European Physical Journal A\",\"FirstCategoryId\":\"4\",\"ListUrlMain\":\"https://link.springer.com/article/10.1140/epja/s10050-024-01381-9\",\"RegionNum\":3,\"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":"The European Physical Journal A","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1140/epja/s10050-024-01381-9","RegionNum":3,"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}
Examination of static fission properties of \(^{236}\)U and \(^{233}\)Th using Cassinian oval parametrization within the macroscopic–microscopic approach
We have conducted a thorough analysis of the potential energy surfaces (PES) in \(^{236}\)U and \(^{233}\)Th using the Cassini-ovals parameterization within the macro–micro approach. We employed the state-of-the-art immersion water flow (IWF) method to study the saddles on four-dimensional energy grids encompassing reflection-asymmetric shapes. For \(^{233}\)Th, we computed the adiabatic potential energy surfaces by minimizing configurations with one blocked neutron within ten levels below and above the Fermi level. Our results show satisfactory agreement with empirical and experimental estimates for both nuclei, specifically regarding the first and second fission barriers. This suggests that our method holds promise in efficiently describing non-compact shapes while reducing the dimensionality of the space without sacrificing accuracy. Interestingly, employing Cassinian oval parameterization fails to reveal a pronounced, hyper-deformed third minimum in the potential energy landscape. Instead, only a shallow third minimum is observed for \(^{233}\)Th, while in \(^{236}\)U, this minimum ultimately vanishes. This finding holds significant importance when considering the modeling of fission cross-sections.
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