中国物理B ›› 2025, Vol. 34 ›› Issue (12): 123101-123101.doi: 10.1088/1674-1056/ade8e3
Ting Liang(梁婷)1,2,3, Min Feng(冯敏)1,2,3, Jin Cao(曹进)1,2,3, Yi-Ming Wang(王艺铭)1,2, Ben-Quan Lu(卢本全)1,2,†, and Hong Chang(常宏)1,2,3,‡
Ting Liang(梁婷)1,2,3, Min Feng(冯敏)1,2,3, Jin Cao(曹进)1,2,3, Yi-Ming Wang(王艺铭)1,2, Ben-Quan Lu(卢本全)1,2,†, and Hong Chang(常宏)1,2,3,‡
摘要: The lifetime of the 5d6s $^{3}$D$_{1}$ clock state in Lu$^{+}$ exhibits a large discrepancy between experimental and theoretical values. To resolve this discrepancy, we perform calculations of the magnetic dipole transition rate between the 5d6s $^{3}$D$_{1}$ and 6s$^{2}$ $^{1}$S$_0$ states using the multi-configuration Dirac-Hartree-Fock method. The effects of electron correlations, Breit interaction, and quantum electrodynamics (QED) corrections on the transition parameters are analyzed systematically. The calculated 5d6s $^{3}$D$_{1}$-6s$^{2}$ $^{1}$S$_0$ magnetic dipole transition rate, $1.69(7)\times 10^{-6}$ s$^{-1}$, shows excellent agreement with the experimental measurement. To accurately determine the lifetime of the $^{3}$D$_{1}$ clock state, the hyperfine-induced electric quadrupole transition rate between the $^{3}$D$_{1}$ and ground states is also calculated. Furthermore, the rates of various transitions between states in the 5d6s configuration are obtained. The lifetimes of the $^{3}$D$_{2,3}$ and $^{1}$D$_{2}$ states are consistent with previous theoretical calculations.
中图分类号: (Ab initio calculations)