SearcharxivSearch

arXiv subjects

Huaxu Dan

Publications and source records attributed to Huaxu Dan.

2 recordsLinked to original sources

Lifetimes of the Metastable $6\mathrm{d}\, ^{2}\mathrm{D}_{5/2}$ and $6\mathrm{d}\, ^{2}\mathrm{D}_{3/2}$ States of Ra$^+$

We report lifetime measurements of the metastable $6\mathrm{d}\, ^{2}\mathrm{D}_{5/2}$ and $6\mathrm{d}\, ^{2}\mathrm{D}_{3/2}$ states of Ra$^+$. The measured lifetimes, $\tau_{5} = $ 303.8(1.5) ms and $\tau_{3} = $ 642(9) ms, are important for optical frequency standards and for benchmarking high-precision relativistic atomic theory. Independent of the reported measurements, the D state lifetimes were calculated using the coupled-cluster single double triple method, in which the coupled-cluster equations for both core and valence triple excitations were solved iteratively. The method was designed for precise prediction of atomic properties, especially for heavy elements, where relativistic and correlation corrections become large, making their treatment more challenging. This Letter presents the first tests of the method for transition properties. Our prediction agrees with experimental values within the uncertainties. The ability to accurately predict the atomic properties of heavy elements is important for many applications, from tests of fundamental symmetries to the development of optical clocks.

physics.atom-ph

Laser Cooling and Hyperfine Measurements of Radium-225 Ions

$^{225}$Ra$^+$ ions (nuclear spin $I=1/2$) have transitions that are first-order insensitive to magnetic field noise, which is advantageous for optical clocks and quantum information science. We report on laser cooling and trapping of $^{225}$Ra$^+$ ions and hyperfine splitting measurements of the ion's $\mathrm{7s}$ $^2\mathrm{S}_{1/2}$, $\mathrm{7p}$ $^2\mathrm{P}_{1/2}$, and $\mathrm{6d}$ $^2\mathrm{D}_{3/2}$ states. We measured the ground state hyperfine constant, $A(\mathrm{S}_{1/2}) =$ $-27.684511052(5)$ $\mathrm{GHz}$, and the quadratic Zeeman coefficient, $C_2 =$ $142.3(1.0)$ $\mathrm{Hz\ G}^{-2}$, of the $^2\mathrm{S}_{1/2} (F=0, m_F = 0) \leftrightarrow~^2\mathrm{S}_{1/2} (F=1, m_{F} = 0)$ transition. Our result addresses a discrepancy in the literature for the ground state hyperfine splitting. We measured the hyperfine constants of the $^2\mathrm{P}_{1/2}$ state, $A(\mathrm{P}_{1/2}) =$ $-5.447(4)$ $\mathrm{GHz}$, and the $^2\mathrm{D}_{3/2}$ state, $A(\mathrm{D}_{3/2}) =$ $-619.7(1.1)$ $\mathrm{MHz}$. We also performed state preparation and measurement using the ground state hyperfine levels and realized a fidelity of $0.9951(9)$.

physics.atom-ph