{"title":"On the multiple-humped fission barriers and half-lives of actinides","authors":"C. Bonilla, G. Royer","doi":"10.1556/APH.25.2006.1.2","DOIUrl":null,"url":null,"abstract":"The energy of actinide nuclei has been determined within a generalized liquid drop model taking into account the proximity energy, the mass and charge asymmetry, an accurate nuclear radius in adding the shell and pairing energies. Double and triple-humped potential barriers appear. The second maximum corresponds to the transition from compact and creviced one-body shapes to two touching ellipsoids. A third minimum and third peak appear in special asymmetric exit channels where one fragment is almost a magic nucleus with a quasi-spherical shape while the other one evolves from oblate to prolate shapes. The heights of the double and triple-humped fission barriers agree precisely with the experimental results in all the actinide region. The predicted half-lives follow the experimental data trend.","PeriodicalId":201208,"journal":{"name":"Acta Physica Hungarica A) Heavy Ion Physics","volume":"98 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2006-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"6","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Acta Physica Hungarica A) Heavy Ion Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1556/APH.25.2006.1.2","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 6
Abstract
The energy of actinide nuclei has been determined within a generalized liquid drop model taking into account the proximity energy, the mass and charge asymmetry, an accurate nuclear radius in adding the shell and pairing energies. Double and triple-humped potential barriers appear. The second maximum corresponds to the transition from compact and creviced one-body shapes to two touching ellipsoids. A third minimum and third peak appear in special asymmetric exit channels where one fragment is almost a magic nucleus with a quasi-spherical shape while the other one evolves from oblate to prolate shapes. The heights of the double and triple-humped fission barriers agree precisely with the experimental results in all the actinide region. The predicted half-lives follow the experimental data trend.