A.A. Valverde , F.G. Kondev , B. Liu , D. Ray , M. Brodeur , D.P. Burdette , N. Callahan , A. Cannon , J.A. Clark , D.E.M. Hoff , R. Orford , W.S. Porter , G. Savard , K.S. Sharma , L. Varriano
{"title":"利用加拿大潘宁陷阱对 A = 133 等值线进行精确质量测量:解决 133Te 的 Qβ- 异常现象","authors":"A.A. Valverde , F.G. Kondev , B. Liu , D. Ray , M. Brodeur , D.P. Burdette , N. Callahan , A. Cannon , J.A. Clark , D.E.M. Hoff , R. Orford , W.S. Porter , G. Savard , K.S. Sharma , L. Varriano","doi":"10.1016/j.physletb.2024.139037","DOIUrl":null,"url":null,"abstract":"<div><div>We report precision mass measurements of <sup>133</sup>Sb, <span><math><msup><mrow></mrow><mrow><mn>133</mn><mi>g</mi><mo>,</mo><mi>m</mi></mrow></msup></math></span>Te, and <span><math><msup><mrow></mrow><mrow><mn>133</mn><mi>g</mi><mo>,</mo><mi>m</mi></mrow></msup></math></span>I, produced at CARIBU at Argonne National Laboratory's ATLAS facility and measured using the Canadian Penning Trap mass spectrometer. These masses clarify an anomaly in the <sup>133</sup>Te <em>β</em>-decay. The masses reported in the 2020 Atomic Mass Evaluation (M. Wang et al., 2021) produce <span><math><msub><mrow><mi>Q</mi></mrow><mrow><msup><mrow><mi>β</mi></mrow><mrow><mo>−</mo></mrow></msup></mrow></msub><mo>(</mo><msup><mrow></mrow><mrow><mn>133</mn></mrow></msup></math></span>Te)=2920(6) keV; however, the highest-lying <sup>133</sup>I level populated in this decay is observed at <span><math><msub><mrow><mi>E</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>=</mo><mn>2935.83</mn><mo>(</mo><mn>15</mn><mo>)</mo></math></span> keV, resulting in an anomalous <span><math><msubsup><mrow><mi>Q</mi></mrow><mrow><msup><mrow><mi>β</mi></mrow><mrow><mo>−</mo></mrow></msup></mrow><mrow><mi>i</mi></mrow></msubsup><mo>=</mo><mo>−</mo><mn>16</mn><mo>(</mo><mn>6</mn><mo>)</mo></math></span> keV. Our new measurements give <span><math><msub><mrow><mi>Q</mi></mrow><mrow><msup><mrow><mi>β</mi></mrow><mrow><mo>−</mo></mrow></msup></mrow></msub><mo>(</mo><mmultiscripts><mrow><mtext>Te</mtext></mrow><mprescripts></mprescripts><none></none><mrow><mn>133</mn></mrow></mmultiscripts><mo>)</mo><mo>=</mo><mn>2934.8</mn><mo>(</mo><mn>11</mn><mo>)</mo></math></span> keV, a factor of five more precise, yielding <span><math><msubsup><mrow><mi>Q</mi></mrow><mrow><mi>β</mi></mrow><mrow><mi>i</mi></mrow></msubsup><mo>=</mo><mo>−</mo><mn>1.0</mn><mo>(</mo><mn>12</mn><mo>)</mo></math></span> keV, a 3<em>σ</em> shift from the previous results. This resolves this anomaly, but indicates further anomalies in our understanding of the structure of this isotope.</div></div>","PeriodicalId":4,"journal":{"name":"ACS Applied Energy Materials","volume":null,"pages":null},"PeriodicalIF":5.4000,"publicationDate":"2024-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0370269324005951/pdfft?md5=a2d63dafc7095842ad61a143db9ace16&pid=1-s2.0-S0370269324005951-main.pdf","citationCount":"0","resultStr":"{\"title\":\"Precise mass measurements of A = 133 isobars with the Canadian Penning Trap: Resolving the Qβ− anomaly at 133Te\",\"authors\":\"A.A. Valverde , F.G. Kondev , B. Liu , D. Ray , M. Brodeur , D.P. Burdette , N. Callahan , A. Cannon , J.A. Clark , D.E.M. Hoff , R. Orford , W.S. Porter , G. Savard , K.S. Sharma , L. Varriano\",\"doi\":\"10.1016/j.physletb.2024.139037\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>We report precision mass measurements of <sup>133</sup>Sb, <span><math><msup><mrow></mrow><mrow><mn>133</mn><mi>g</mi><mo>,</mo><mi>m</mi></mrow></msup></math></span>Te, and <span><math><msup><mrow></mrow><mrow><mn>133</mn><mi>g</mi><mo>,</mo><mi>m</mi></mrow></msup></math></span>I, produced at CARIBU at Argonne National Laboratory's ATLAS facility and measured using the Canadian Penning Trap mass spectrometer. These masses clarify an anomaly in the <sup>133</sup>Te <em>β</em>-decay. The masses reported in the 2020 Atomic Mass Evaluation (M. Wang et al., 2021) produce <span><math><msub><mrow><mi>Q</mi></mrow><mrow><msup><mrow><mi>β</mi></mrow><mrow><mo>−</mo></mrow></msup></mrow></msub><mo>(</mo><msup><mrow></mrow><mrow><mn>133</mn></mrow></msup></math></span>Te)=2920(6) keV; however, the highest-lying <sup>133</sup>I level populated in this decay is observed at <span><math><msub><mrow><mi>E</mi></mrow><mrow><mi>i</mi></mrow></msub><mo>=</mo><mn>2935.83</mn><mo>(</mo><mn>15</mn><mo>)</mo></math></span> keV, resulting in an anomalous <span><math><msubsup><mrow><mi>Q</mi></mrow><mrow><msup><mrow><mi>β</mi></mrow><mrow><mo>−</mo></mrow></msup></mrow><mrow><mi>i</mi></mrow></msubsup><mo>=</mo><mo>−</mo><mn>16</mn><mo>(</mo><mn>6</mn><mo>)</mo></math></span> keV. Our new measurements give <span><math><msub><mrow><mi>Q</mi></mrow><mrow><msup><mrow><mi>β</mi></mrow><mrow><mo>−</mo></mrow></msup></mrow></msub><mo>(</mo><mmultiscripts><mrow><mtext>Te</mtext></mrow><mprescripts></mprescripts><none></none><mrow><mn>133</mn></mrow></mmultiscripts><mo>)</mo><mo>=</mo><mn>2934.8</mn><mo>(</mo><mn>11</mn><mo>)</mo></math></span> keV, a factor of five more precise, yielding <span><math><msubsup><mrow><mi>Q</mi></mrow><mrow><mi>β</mi></mrow><mrow><mi>i</mi></mrow></msubsup><mo>=</mo><mo>−</mo><mn>1.0</mn><mo>(</mo><mn>12</mn><mo>)</mo></math></span> keV, a 3<em>σ</em> shift from the previous results. This resolves this anomaly, but indicates further anomalies in our understanding of the structure of this isotope.</div></div>\",\"PeriodicalId\":4,\"journal\":{\"name\":\"ACS Applied Energy Materials\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":5.4000,\"publicationDate\":\"2024-09-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://www.sciencedirect.com/science/article/pii/S0370269324005951/pdfft?md5=a2d63dafc7095842ad61a143db9ace16&pid=1-s2.0-S0370269324005951-main.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"ACS Applied Energy Materials\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0370269324005951\",\"RegionNum\":3,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Energy Materials","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0370269324005951","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
Precise mass measurements of A = 133 isobars with the Canadian Penning Trap: Resolving the Qβ− anomaly at 133Te
We report precision mass measurements of 133Sb, Te, and I, produced at CARIBU at Argonne National Laboratory's ATLAS facility and measured using the Canadian Penning Trap mass spectrometer. These masses clarify an anomaly in the 133Te β-decay. The masses reported in the 2020 Atomic Mass Evaluation (M. Wang et al., 2021) produce Te)=2920(6) keV; however, the highest-lying 133I level populated in this decay is observed at keV, resulting in an anomalous keV. Our new measurements give keV, a factor of five more precise, yielding keV, a 3σ shift from the previous results. This resolves this anomaly, but indicates further anomalies in our understanding of the structure of this isotope.
期刊介绍:
ACS Applied Energy Materials is an interdisciplinary journal publishing original research covering all aspects of materials, engineering, chemistry, physics and biology relevant to energy conversion and storage. The journal is devoted to reports of new and original experimental and theoretical research of an applied nature that integrate knowledge in the areas of materials, engineering, physics, bioscience, and chemistry into important energy applications.