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Diffuse laser cooling based on the 6P3/2 excited state of rubidium atoms via 420 nm blue light

Jia Zhang1, Xun Gao1, Zheng Xiao1, Xiaolei Guan1, Ruihang Chen1, Mengyuan Han1, Tiantian Shi2,3,*, and Jingbiao Chen1,2,4

  • 1Institute of Quantum Electronics, School of Electronics, Peking University, Beijing 100871, China
  • 2National Key Laboratory of Advanced Micro and Nano Manufacture Technology, School of Integrated Circuits, Peking University, Beijing 100871, China
  • 3Beijing Advanced Innovation Center for Integrated Circuits, Beijing 100871, China
  • 4Hefei National Laboratory, Hefei 230088, China

  • *Contact author: tts@pku.edu.cn

Phys. Rev. Research 8, 033293 – Published 10 September, 2026

DOI: https://doi.org/10.1103/4jtk-471b

Abstract

To date, the laser cooling of rubidium atoms has inevitably relied on 780 nm cooling light corresponding to the first excited state 5P3/2. Here, we demonstrate diffuse laser cooling of Rb87 atoms using the 420 nm 5S1/26P3/2 transition without a preceding 780 nm cooling stage. A high-power 420nm 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 1.4×1011m3. 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.

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