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We realize narrow-linewidth magneto-optical traps of ⁴⁶Ti, ⁴⁸Ti and ⁵⁰Ti atoms based on a 1040 nm-wavelength transition, cooling atoms to a minimum temperature in one dimension of Tz=990(20) nK and a three-dimensional temperature of T₃D=1.28(7) $μ$K. Atoms are pre-cooled in a broad-line magneto-optical trap and then transferred with about 25% efficiency to the narrow-line trap. We operate the narrow-line trap in two stages over 85 ms. First, a single cooling beam, blue-detuned from the narrow-linewidth atomic resonance, optically pumps and traps the atoms on a two-dimensional surface where the Zeeman shift from the applied spherical quadrupole magnetic field brings the light nearly to resonance. Second, four additional beams, counter-propagating in the transverse directions, cool and compress the atoms in all dimensions. The high magnetic moment of the laser cooling state makes the dynamics of the narrow-line titanium trap similar to those of other magnetic atoms. We measure the lifetime of the excited state of the transition to be $τ=8.2(9)$ $μ$s, indicating a transition linewidth of $γ/2π=20(2)$ kHz, and also measure isotope shifts on the narrow-line transition. We use Stern-Gerlach separation on the ultracold Ti gas to measure the mJ-distribution in the narrow-line magneto-optical trap, finding over 98% of the atoms in the stretched spin state.
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Duim et al. (2026) studied this question.
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