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Physical Review A

Measurement of lifetime, hyperfine splitting, and Landé g J factor of the F 5 / 2 2 state in Yb + 171

Pavel Sidorov, Pavel A. Kamenskikh, Ilya Gerasin, Alexander S. Borisenko, Ilia V. Zalivako, Ilya A. Semerikov, Ksenia Yu. Khabarova, N. Kolachevsky

Published Mar 19, 2026• 2 citations
Publisher
DOI
10.1103/kkbx-nzg2

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We report the determination of the Land\'e ${g}_{J}$ factor and Zeeman coefficients for the ground-state of ${}^{171}{\mathrm{Yb}}^{+}$, relevant to microwave quantum frequency standards (QFSs). The ${g}_{J}$ factor is obtained by using two independent methods, the multiconfiguration Dirac-Hartree-Fock and multireference configuration-interaction methods, yielding a consistent value of $2.002\phantom{\rule{0.16em}{0ex}}615(70)$. The first- and second-order Zeeman coefficients are determined as $14\phantom{\rule{0.16em}{0ex}}010.78(49)\phantom{\rule{4pt}{0ex}}\mathrm{Hz}/\textmu{}\mathrm{T}$ and $31.0869(22)\phantom{\rule{4pt}{0ex}}\mathrm{mHz}/\textmu{}{\mathrm{T}}^{2}$, respectively, based on the calculated ${g}_{J}$ factor. These coefficients enable reduced magnetic-field-induced uncertainties, improving the accuracy of the ${}^{171}{\mathrm{Yb}}^{+}$ microwave QFSs. The results reported in this work also offer potential for improved constraints on variations in fundamental constants through frequency comparisons and advancing trapped-ion quantum computers based on the ground-state hyperfine splitting of ${}^{171}{\mathrm{Yb}}^{+}$.

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We report spectroscopic and time-resolved experimental observations to characterize the [ Xe ] 4 f 13 ( F 5 / 2 o 2 ) 5 d 6 s ( D 1 ) 1 [ 5 / 2 ] 5 / 2 o state in Yb + 172 ions. We access this state from the metastable 4 f 14 5 d ( D 3 / 2 , 5 / 2 2 ) manifold and observe an unexpectedly long lifetime of τ = 37.9 ( 9 ) µ s that allows visible Rabi oscillations and resolved-sideband spectroscopy. Using a combination of coherent population dynamics, high-fidelity detection and heralded state preparation, and optical pumping methods, we measure the branching ratios to the D 3 / 2 2 , D 5 / 2 2 , and S 1 / 2 2 states to be 0.359 ( 2 ) , 0.639(2), and 0.0023 ( 16 ) , respectively. The branching ratio to the 4 f 13 6 s 2 ( F 2 7 / 2 ) is compatible with zero within our experimental resolution. We also report measurements of Landé g -factor of the 1 [ 5

arXiv:2506.04320•Physical Review Research•Sep 23, 2025•1 citation
Determination of Landé gJg_JgJ​ factor and Zeeman coefficients in ground-state 171^{171}171Yb+^++ and their applications to quantum frequency standards
We report the determination of the Landé gJg_JgJ​ factor and Zeeman coefficients for the ground-state of 171^{171}171Yb+^++, relevant to microwave quantum frequency standards (QFSs). The gJg_JgJ​ factor is obtained by using two independent methods: multiconfiguration Dirac-Hartree-Fock and multireference configuration interaction, yielding a consistent value of 2.002615(70). The first- and second-order Zeeman coefficients are determined as 14,010.78(49) Hz/μμμT and 31.0869(22) mHz/μμμT2^22, respectively, based on the calculated gJg_JgJ​ factor. These coefficients enable reduced magnetic-field-induced uncertainties, improving the accuracy of the 171^{171}171Yb+^++ microwave QFSs. The results reported in this work also offer potential for improved constraints on variations in fundamental constants through frequency comparisons, and advancing trapped-ion quantum computers based on the ground-state hyperfine splitting of 171^{171}171Yb+^++.
We report the determination of the Land\'e gJ{g}_{J}gJ​ factor and Zeeman coefficients for the ground-state of 171Yb+{}^{171}{\mathrm{Yb}}^{+}171Yb+, relevant to microwave quantum frequency standards (QFSs). The gJ{g}_{J}gJ​ factor is obtained by using two independent methods, the multiconfiguration Dirac-Hartree-Fock and multireference configuration-interaction methods, yielding a consistent value of 2.002615(70)2.002\phantom{\rule{0.16em}{0ex}}615(70)2.002615(70). The first- and second-order Zeeman coefficients are determined as $14\phantom{\rule{0.16em}{0ex}}010.78(49)\phantom{\rule{4pt}{0ex}}\mathrm{Hz}/\textmu{}\mathrm{T}$ and $31.0869(22)\phantom{\rule{4pt}{0ex}}\mathrm{mHz}/\textmu{}{\mathrm{T}}^{2}$, respectively, based on the calculated gJ{g}_{J}gJ​ factor. These coefficients enable reduced magnetic-field-induced uncertainties, improving the accuracy of the 171Yb+{}^{171}{\mathrm{Yb}}^{+}171Yb+ microwave QFSs. The results reported in this work also offer potential for improved constraints on variations in fundamental constants through frequency comparisons and advancing trapped-ion quantum computers based on the ground-state hyperfine splitting of 171Yb+{}^{171}{\mathrm{Yb}}^{+}171Yb+.
We report spectroscopic and time-resolved experimental observations to characterize the [ Xe ] 4 f 13 ( F 5 / 2 o 2 ) 5 d 6 s ( D 1 ) 1 [ 5 / 2 ] 5 / 2 o state in Yb + 172 ions. We access this state from the metastable 4 f 14 5 d ( D 3 / 2 , 5 / 2 2 ) manifold and observe an unexpectedly long lifetime of τ = 37.9 ( 9 ) µ s that allows visible Rabi oscillations and resolved-sideband spectroscopy. Using a combination of coherent population dynamics, high-fidelity detection and heralded state preparation, and optical pumping methods, we measure the branching ratios to the D 3 / 2 2 , D 5 / 2 2 , and S 1 / 2 2 states to be 0.359 ( 2 ) , 0.639(2), and 0.0023 ( 16 ) , respectively. The branching ratio to the 4 f 13 6 s 2 ( F 2 7 / 2 ) is compatible with zero within our experimental resolution. We also report measurements of Landé g -factor of the 1 [ 5