{"title":"更高的禁区独特 $β^-$ 衰变跃迁和壳模型解释","authors":"Archana Saxena, Praveen C. Srivastava","doi":"arxiv-2409.11244","DOIUrl":null,"url":null,"abstract":"In the present work, we have predicted the half-lives for the $\\beta^{-}$\ndecay for higher forbidden unique transitions in the mass range of nuclei from\nA = 40-138. For these transitions, the experimental data for half-lives are not\navailable except for a few cases. The calculations for half-lives are performed\nwithin the framework of the nuclear shell model (SM). We have used the\neffective interactions sdpf-mu, gxpf1a, gwbxg, G-matrix, snet, sn100pn, and\njj56pnb to perform the SM calculations in different mass regions. A\ncomprehensive discussion has been made between the SM-predicted half-lives and\nthe scaled half-lives from proton-neutron quasiparticle random-phase\napproximation (pnQRPA). The results of the present study will be useful to plan\nnew experiments to measure half-lives for these higher forbidden unique\n$\\beta^{-}$ transitions.","PeriodicalId":501573,"journal":{"name":"arXiv - PHYS - Nuclear Theory","volume":"64 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Higher forbidden unique $β^-$ decay transitions and shell-model interpretation\",\"authors\":\"Archana Saxena, Praveen C. Srivastava\",\"doi\":\"arxiv-2409.11244\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In the present work, we have predicted the half-lives for the $\\\\beta^{-}$\\ndecay for higher forbidden unique transitions in the mass range of nuclei from\\nA = 40-138. For these transitions, the experimental data for half-lives are not\\navailable except for a few cases. The calculations for half-lives are performed\\nwithin the framework of the nuclear shell model (SM). We have used the\\neffective interactions sdpf-mu, gxpf1a, gwbxg, G-matrix, snet, sn100pn, and\\njj56pnb to perform the SM calculations in different mass regions. A\\ncomprehensive discussion has been made between the SM-predicted half-lives and\\nthe scaled half-lives from proton-neutron quasiparticle random-phase\\napproximation (pnQRPA). The results of the present study will be useful to plan\\nnew experiments to measure half-lives for these higher forbidden unique\\n$\\\\beta^{-}$ transitions.\",\"PeriodicalId\":501573,\"journal\":{\"name\":\"arXiv - PHYS - Nuclear Theory\",\"volume\":\"64 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Nuclear Theory\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.11244\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Nuclear Theory","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.11244","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
在本研究中,我们预测了原子核质量范围从A = 40-138的高禁唯一跃迁的$\beta^{-}$衰变的半衰期。对于这些跃迁,除少数情况外,没有半衰期的实验数据。半衰期的计算是在核壳模型(SM)的框架内进行的。我们使用了有效的相互作用 sdpf-mu、gxpf1a、gwbxg、G-matrix、snet、sn100pn 和 jj56pnb 来进行不同质量区域的 SM 计算。对 SM 预测的半衰期和质子-中子准粒子随机相位逼近(pnQRPA)的缩放半衰期进行了全面讨论。本研究的结果将有助于规划新的实验,以测量这些更高的禁止的独特$\beta^{-}$转变的半衰期。
Higher forbidden unique $β^-$ decay transitions and shell-model interpretation
In the present work, we have predicted the half-lives for the $\beta^{-}$
decay for higher forbidden unique transitions in the mass range of nuclei from
A = 40-138. For these transitions, the experimental data for half-lives are not
available except for a few cases. The calculations for half-lives are performed
within the framework of the nuclear shell model (SM). We have used the
effective interactions sdpf-mu, gxpf1a, gwbxg, G-matrix, snet, sn100pn, and
jj56pnb to perform the SM calculations in different mass regions. A
comprehensive discussion has been made between the SM-predicted half-lives and
the scaled half-lives from proton-neutron quasiparticle random-phase
approximation (pnQRPA). The results of the present study will be useful to plan
new experiments to measure half-lives for these higher forbidden unique
$\beta^{-}$ transitions.