Blue laser cooling transitions in Tm I

TL;DR

This study identifies and characterizes laser cooling transitions in thulium-169, demonstrating a promising transition at 410.6 nm with minimal leak rate suitable for efficient cooling, and explores related atomic properties for potential clock applications.

Contribution

The paper provides detailed measurements of hyperfine structures, transition rates, and decay pathways for Tm I laser cooling candidates, including a transition with very low leak rate for efficient cooling.

Findings

The 410.6 nm transition has an optical leak rate less than 2×10⁻⁵.

The excited state lifetimes are measured as 15.9(8) ns and 48(6) ns.

The magnetic-dipole transition rate at 1.14 μm is estimated as 7(2) s⁻¹.

Abstract

We have studied possible candidates for laser cooling transitions in $^{169}$Tm in the spectral region 410 -- 420 nm. By means of saturation absorption spectroscopy we have measured the hyperfine structure and rates of two nearly closed cycling transitions from the ground state $4\textrm{f}^{13}6\textrm{s}^2(^2\textrm{F}_0)(J_g=7/2)$ to upper states $4\textrm{f}^{12}(^3\textrm{H}_5)5\textrm{d}_{3/2}6\textrm{s}^2(J_e=9/2)$ at 410.6 nm and $4\textrm{f}^{12}(^3\textrm{F}_4)5\textrm{d}_{5/2}6\textrm{s}^2(J_e=9/2)$ at 420.4 nm and evaluated the life times of the excited levels as 15.9(8) ns and 48(6) ns respectively. Decay rates from these levels to neighboring opposite-parity levels are evaluated by means of Hartree-Fock calculations. We conclude, that the strong transition at 410.6 nm has an optical leak rate of less then $2\cdot10^{-5}$ and can be used for efficient laser cooling of $^{169}$Tm from a thermal atomic beam. The hyperfine structure of two other even-parity levels which can be excited from the ground state at 409.5 nm and 418.9 nm is also measured by the same technique. In addition we give a calculated value of $7(2)$ s$^{-1}$ for the rate of magnetic-dipole transition at 1.14 $\mu$m between the fine structure levels $(J_g=7/2)\leftrightarrow(J'_g=5/2)$ of the ground state which can be considered as a candidate for applications in atomic clocks.