Measurement of Hyperfine Structure and the Zemach Radius in ^{6}Li^{+} Using Optical Ramsey Technique
We investigate the 2^{3}S_{1}-2^{3}P_{J} (J=0, 1, 2) transitions in ^{6}Li^{+} using the optical Ramsey technique and achieve the most precise values of the hyperfine splittings of the 2^{3}S_{1} and 2^{3}P_{J} states, with smallest uncertainty of about 10 kHz. The present results reduce the uncertainties of previous experiments by a factor of 5 for the 2^{3}S_{1} state and a factor of 50 for the 2^{3}P_{J} states, and are in better agreement with theoretical values. Combining our measured hyperfine intervals of the 2^{3}S_{1} state with the latest quantum electrodynamic (QED) calculations, the improved Zemach radius of the ^{6}Li nucleus is determined to be 2.44(2) fm, with the uncertainty entirely due to the uncalculated QED effects of order mα^{7}. The result is in sharp disagreement with the value 3.71(16) fm determined from simple models of the nuclear charge and magnetization distribution. We call for a more definitive nuclear physics value of the ^{6}Li Zemach radius.
Medienart: |
E-Artikel |
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Erscheinungsjahr: |
2023 |
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Erschienen: |
2023 |
Enthalten in: |
Zur Gesamtaufnahme - volume:131 |
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Enthalten in: |
Physical review letters - 131(2023), 10 vom: 08. Sept., Seite 103002 |
Sprache: |
Englisch |
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Beteiligte Personen: |
Sun, Wei [VerfasserIn] |
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Anmerkungen: |
Date Revised 22.09.2023 published: Print Citation Status PubMed-not-MEDLINE |
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doi: |
10.1103/PhysRevLett.131.103002 |
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funding: |
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Förderinstitution / Projekttitel: |
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PPN (Katalog-ID): |
NLM362358834 |
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520 | |a We investigate the 2^{3}S_{1}-2^{3}P_{J} (J=0, 1, 2) transitions in ^{6}Li^{+} using the optical Ramsey technique and achieve the most precise values of the hyperfine splittings of the 2^{3}S_{1} and 2^{3}P_{J} states, with smallest uncertainty of about 10 kHz. The present results reduce the uncertainties of previous experiments by a factor of 5 for the 2^{3}S_{1} state and a factor of 50 for the 2^{3}P_{J} states, and are in better agreement with theoretical values. Combining our measured hyperfine intervals of the 2^{3}S_{1} state with the latest quantum electrodynamic (QED) calculations, the improved Zemach radius of the ^{6}Li nucleus is determined to be 2.44(2) fm, with the uncertainty entirely due to the uncalculated QED effects of order mα^{7}. The result is in sharp disagreement with the value 3.71(16) fm determined from simple models of the nuclear charge and magnetization distribution. We call for a more definitive nuclear physics value of the ^{6}Li Zemach radius | ||
650 | 4 | |a Journal Article | |
700 | 1 | |a Zhang, Pei-Pei |e verfasserin |4 aut | |
700 | 1 | |a Zhou, Peng-Peng |e verfasserin |4 aut | |
700 | 1 | |a Chen, Shao-Long |e verfasserin |4 aut | |
700 | 1 | |a Zhou, Zhi-Qiang |e verfasserin |4 aut | |
700 | 1 | |a Huang, Yao |e verfasserin |4 aut | |
700 | 1 | |a Qi, Xiao-Qiu |e verfasserin |4 aut | |
700 | 1 | |a Yan, Zong-Chao |e verfasserin |4 aut | |
700 | 1 | |a Shi, Ting-Yun |e verfasserin |4 aut | |
700 | 1 | |a Drake, G W F |e verfasserin |4 aut | |
700 | 1 | |a Zhong, Zhen-Xiang |e verfasserin |4 aut | |
700 | 1 | |a Guan, Hua |e verfasserin |4 aut | |
700 | 1 | |a Gao, Ke-Lin |e verfasserin |4 aut | |
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