{"title":"A=149等压线的核结构和衰变数据","authors":"Balraj Singh , Jun Chen","doi":"10.1016/j.nds.2022.10.001","DOIUrl":null,"url":null,"abstract":"<div><p>Experimental nuclear structure and decay data are evaluated for all the 17 known nuclides of mass 149 (Xe, Cs, Ba, La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb). Detailed compiled and evaluated spectroscopic information is presented for each reaction and decay dataset, and recommended values are provided for level properties, <em>α</em>, <em>β</em> and <em>γ</em> radiations, and other spectroscopic parameters, based on an evaluation of all the available experimental data for A=149 isobaric nuclides. Although large amounts of nuclear spectroscopic data are available for nuclides of A=149, yet large gaps in knowledge exist, as described below. For the lowest atomic number nuclide <sup>149</sup>Xe, only the isotopic identification has been made, with no data for its ground-state half-life. For <sup>149</sup>Cs, <sup>149</sup>Tm and <sup>149</sup>Yb information is available for only the respective ground states. For <sup>149</sup>Ba, <sup>149</sup>La and <sup>149</sup>Er, limited data exist for excited states. Many of the decay schemes of radioactive nuclei of A=149 are considered as incomplete, either due to large energy differences between the highest observed excited states in daughter nuclides and the respective Q-values, or due to the lack of confirmed <em>γ</em>-ray data, as listed below: <sup>149</sup>Cs → <sup>149</sup>Ba, <sup>149</sup>Ba → <sup>149</sup>La, <sup>149</sup>La → <sup>149</sup>Ce, <sup>149</sup>Ce → <sup>149</sup>Pr, <sup>149</sup>Pr → <sup>149</sup>Nd, <sup>149</sup>Tb(4.17 min) → <sup>149</sup>Gd, <sup>149</sup>Ho(21.0 s and 56 s) → <sup>149</sup>Dy, <sup>149</sup>Er(4 s and 9.6 s) → <sup>149</sup>Ho, and <sup>149</sup>Tm → <sup>149</sup>Er. No data exist for the decay of <sup>149</sup>Yb to <sup>149</sup>Tm. Data for half-lives of the excited states in this mass chain are generally lacking as given below by the number of excited levels of known half-life / approximate number of known levels in a nuclide: 2/17 for <sup>149</sup>Ba, 0/18 for <sup>149</sup>La, 3/53 for <sup>149</sup>Ce, 3/44 for <sup>149</sup>Pr, 17/110 for <sup>149</sup>Nd, 9/90 for <sup>149</sup>Pm, 10/210 for <sup>149</sup>Sm, 2/125 for <sup>149</sup>Eu, 6/270 for <sup>149</sup>Gd, 5/200 for <sup>149</sup>Tb, 3/80 for <sup>149</sup>Dy, 3/90 for <sup>149</sup>Ho, and 3/14 for <sup>149</sup>Er. This work supersedes earlier evaluations of A=149 nuclides published by 2004Si16, 1994Si18, 1985Sz01 and 1976Ho17.</p></div>","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"185 ","pages":"Pages 2-559"},"PeriodicalIF":2.8000,"publicationDate":"2022-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Nuclear Structure and Decay Data for A=149 Isobars\",\"authors\":\"Balraj Singh , Jun Chen\",\"doi\":\"10.1016/j.nds.2022.10.001\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Experimental nuclear structure and decay data are evaluated for all the 17 known nuclides of mass 149 (Xe, Cs, Ba, La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb). Detailed compiled and evaluated spectroscopic information is presented for each reaction and decay dataset, and recommended values are provided for level properties, <em>α</em>, <em>β</em> and <em>γ</em> radiations, and other spectroscopic parameters, based on an evaluation of all the available experimental data for A=149 isobaric nuclides. Although large amounts of nuclear spectroscopic data are available for nuclides of A=149, yet large gaps in knowledge exist, as described below. For the lowest atomic number nuclide <sup>149</sup>Xe, only the isotopic identification has been made, with no data for its ground-state half-life. For <sup>149</sup>Cs, <sup>149</sup>Tm and <sup>149</sup>Yb information is available for only the respective ground states. For <sup>149</sup>Ba, <sup>149</sup>La and <sup>149</sup>Er, limited data exist for excited states. Many of the decay schemes of radioactive nuclei of A=149 are considered as incomplete, either due to large energy differences between the highest observed excited states in daughter nuclides and the respective Q-values, or due to the lack of confirmed <em>γ</em>-ray data, as listed below: <sup>149</sup>Cs → <sup>149</sup>Ba, <sup>149</sup>Ba → <sup>149</sup>La, <sup>149</sup>La → <sup>149</sup>Ce, <sup>149</sup>Ce → <sup>149</sup>Pr, <sup>149</sup>Pr → <sup>149</sup>Nd, <sup>149</sup>Tb(4.17 min) → <sup>149</sup>Gd, <sup>149</sup>Ho(21.0 s and 56 s) → <sup>149</sup>Dy, <sup>149</sup>Er(4 s and 9.6 s) → <sup>149</sup>Ho, and <sup>149</sup>Tm → <sup>149</sup>Er. No data exist for the decay of <sup>149</sup>Yb to <sup>149</sup>Tm. Data for half-lives of the excited states in this mass chain are generally lacking as given below by the number of excited levels of known half-life / approximate number of known levels in a nuclide: 2/17 for <sup>149</sup>Ba, 0/18 for <sup>149</sup>La, 3/53 for <sup>149</sup>Ce, 3/44 for <sup>149</sup>Pr, 17/110 for <sup>149</sup>Nd, 9/90 for <sup>149</sup>Pm, 10/210 for <sup>149</sup>Sm, 2/125 for <sup>149</sup>Eu, 6/270 for <sup>149</sup>Gd, 5/200 for <sup>149</sup>Tb, 3/80 for <sup>149</sup>Dy, 3/90 for <sup>149</sup>Ho, and 3/14 for <sup>149</sup>Er. This work supersedes earlier evaluations of A=149 nuclides published by 2004Si16, 1994Si18, 1985Sz01 and 1976Ho17.</p></div>\",\"PeriodicalId\":49735,\"journal\":{\"name\":\"Nuclear Data Sheets\",\"volume\":\"185 \",\"pages\":\"Pages 2-559\"},\"PeriodicalIF\":2.8000,\"publicationDate\":\"2022-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Data Sheets\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0090375222000461\",\"RegionNum\":1,\"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":"Nuclear Data Sheets","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0090375222000461","RegionNum":1,"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}
引用次数: 0
摘要
对所有17种已知质量为149的核素(Xe、Cs、Ba、La、Ce、Pr、Nd、Pm、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、Yb)的实验核结构和衰变数据进行了评估。详细编译和评估了每个反应和衰变数据集的光谱信息,并根据对A=149等压核素的所有可用实验数据的评估,提供了能级性质,α, β和γ辐射以及其他光谱参数的推荐值。虽然对于A=149的核素有大量的核光谱数据,但是在知识上存在很大的空白,如下所述。对于原子序数最低的核素149Xe,只进行了同位素鉴定,没有基态半衰期的数据。对于149Cs、149Tm和149Yb,只有各自基态的信息可用。对于149Ba、149La和149Er,激发态数据有限。许多放射性原子核的衰变模式= 149的视为不完整,要么由于大型能源观察最高激发态之间的差异在女儿核素和各自的q值,或由于缺乏γ射线数据确认,如下所列:149 cs→149 ba ba 149→149年洛杉矶,149年洛杉矶→公元149年,公元149年→149公关,公关149→149,149 tb(4.17分钟)→149 gd 149 ho(21.0和56个年代)→149 dy, 149 er(4和9.6年代)→149,和149年的tm→149 er。没有149Yb到149Tm衰变的数据。该质量链中激发态的半衰期数据一般缺乏,如下所示:已知半衰期的激发态能级数/核素已知半衰期的大致能级数:149Ba为2/17,149La为0/18,149Ce为3/53,149Pr为3/44,149Nd为17/110,149Pm为9/90,149Sm为10/210,149Eu为2/125,149Gd为6/270,149Tb为5/200,149Dy为3/80,149Ho为3/90,149Er为3/14。这项工作取代了2004年4月16日、1994年4月18日、1985年5月1日和1976年6月17日发表的对A=149核素的早期评价。
Nuclear Structure and Decay Data for A=149 Isobars
Experimental nuclear structure and decay data are evaluated for all the 17 known nuclides of mass 149 (Xe, Cs, Ba, La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb). Detailed compiled and evaluated spectroscopic information is presented for each reaction and decay dataset, and recommended values are provided for level properties, α, β and γ radiations, and other spectroscopic parameters, based on an evaluation of all the available experimental data for A=149 isobaric nuclides. Although large amounts of nuclear spectroscopic data are available for nuclides of A=149, yet large gaps in knowledge exist, as described below. For the lowest atomic number nuclide 149Xe, only the isotopic identification has been made, with no data for its ground-state half-life. For 149Cs, 149Tm and 149Yb information is available for only the respective ground states. For 149Ba, 149La and 149Er, limited data exist for excited states. Many of the decay schemes of radioactive nuclei of A=149 are considered as incomplete, either due to large energy differences between the highest observed excited states in daughter nuclides and the respective Q-values, or due to the lack of confirmed γ-ray data, as listed below: 149Cs → 149Ba, 149Ba → 149La, 149La → 149Ce, 149Ce → 149Pr, 149Pr → 149Nd, 149Tb(4.17 min) → 149Gd, 149Ho(21.0 s and 56 s) → 149Dy, 149Er(4 s and 9.6 s) → 149Ho, and 149Tm → 149Er. No data exist for the decay of 149Yb to 149Tm. Data for half-lives of the excited states in this mass chain are generally lacking as given below by the number of excited levels of known half-life / approximate number of known levels in a nuclide: 2/17 for 149Ba, 0/18 for 149La, 3/53 for 149Ce, 3/44 for 149Pr, 17/110 for 149Nd, 9/90 for 149Pm, 10/210 for 149Sm, 2/125 for 149Eu, 6/270 for 149Gd, 5/200 for 149Tb, 3/80 for 149Dy, 3/90 for 149Ho, and 3/14 for 149Er. This work supersedes earlier evaluations of A=149 nuclides published by 2004Si16, 1994Si18, 1985Sz01 and 1976Ho17.
期刊介绍:
The Nuclear Data Sheets are current and are published monthly. They are devoted to compilation and evaluations of experimental and theoretical results in Nuclear Physics. The journal is mostly produced from Evaluated Nuclear Structure Data File (ENSDF), a computer file maintained by the US National Nuclear Data Center