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Physical Review A

Two-color laser cooling with the rubidium optical clock transition

Wictor C. Magno, Flávio C. Cruz

Published Jun 8, 2026• 0 citations
Publisher
DOI
10.1103/vbbt-8lsg

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To date, the laser cooling of rubidium atoms has inevitably relied on 780 nm cooling light corresponding to the first excited state 5 P 3 / 2 . Here, we demonstrate diffuse laser cooling of Rb 87 atoms using the 420 nm 5 S 1 / 2 → 6 P 3 / 2 transition without a preceding 780 nm cooling stage. A high-power 420 nm laser is used as the cooling light to produce cold atoms in a 1-m-long diffuse-cooling cell. Absorption spectroscopy yields a cold-atom density of approximately 1.4 × 10 11 m − 3 . We compare the cooling performance of the 420 nm and conventional 780 nm diffuse-cooling schemes and verify the feasibility of using the high-excited-state transition as an independent cooling channel in this large-volume diffuse-cooling system. This approach provides an alternative cooling/pumping pathway for continuous cold-atom active optical clocks, where compatibility with the clock-lasing process and reduced cooling-light-induced perturbations are important. It is also expected to open up research directions and application prospects in frontier fields such as Rydberg atoms, quantum information, and so on.

arXiv:2511.16220•Physical Review Research•Aug 18, 2026•0 citations
To date, the laser cooling of rubidium atoms has inevitably relied on 780 nm cooling light corresponding to the first excited state 5 P 3 / 2 . Here, we demonstrate diffuse laser cooling of Rb 87 atoms using the 420 nm 5 S 1 / 2 → 6 P 3 / 2 transition without a preceding 780 nm cooling stage. A high-power 420 nm laser is used as the cooling light to produce cold atoms in a 1-m-long diffuse-cooling cell. Absorption spectroscopy yields a cold-atom density of approximately 1.4 × 10 11 m − 3 . We compare the cooling performance of the 420 nm and conventional 780 nm diffuse-cooling schemes and verify the feasibility of using the high-excited-state transition as an independent cooling channel in this large-volume diffuse-cooling system. This approach provides an alternative cooling/pumping pathway for continuous cold-atom active optical clocks, where compatibility with the clock-lasing process and reduced cooling-light-induced perturbations are important. It is also expected to open up research directions and application prospects in frontier fields such as Rydberg atoms, quantum information, and so on.