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    Magic wavelengths for optical clock transitions in Rb85, Cs133, and Fr223 in visible-near-infrared spectrum

    Jyoti1,2,*, Mandeep Kaur3, Tiantian Shi4, and Jingbiao Chen1,2,†

    • 1State Key Laboratory of Photonics and Communications, Institute of Quantum Electronics, School of Electronics, Peking University, Beijing 100871, People's Republic of China
    • 2Hefei National Laboratory, Anhui, Hefei 230088, People's Republic of China
    • 3Department of Physics, University Institute of Sciences, Chandigarh University, Sahibzada Ajit Singh Nagar (Mohali), Punjab 140413, India
    • 4National Key Laboratory of Advanced Micro and Nano Manufacture Technology, School of Integrated Circuits, Peking University, Beijing 100871, People's Republic of China

    • *Contact author: arora.jyoti326@gmail.com
    • †Contact author: jbchen@pku.edu.cn

    Phys. Rev. A 112, 063106 – Published 3 December, 2025

    DOI: https://doi.org/10.1103/9yy9-v6v1

    Abstract

    Neutral atom manipulation along with the modern laser cooling and trapping techniques have revolutionized the field of atomic physics, enabling innovation among atomic clocks as well as in the study of parity violation and the search for electron electric-dipole moment and nuclear anapole moment. The realization of highly precise and accurate atomic clocks evidently requires high signal-to-noise ratio, which is inversely proportional to Allan deviation. Keeping this in mind, we have calculated magic wavelengths (λmagic) for optical clock transitions in Rb85, Cs133, and Fr223 atoms, viz, 5S1/2−6P1/2,3/2, 6S1/2−7P1/2,3/2, and 7S1/2−8P1/2,3/2, respectively, particularly in the visible-near-infrared spectrum, owing to the fact that Allan deviation rapidly decreases with higher wavelengths of the electromagnetic spectrum, making them more acceptable for newer navigation systems, quantum computation devices as well as tools for high-precision experiments. In this study, we also recommend investigating near-resonant λmagic for Rb85 [420.81(2), 418.21(4),421.390(4), and 417.67 nm] and Cs133 [458.84(4) nm], utilizing dual-purpose lasers of ≈420 nm and ≈459 nm for cooling and pumping of atoms for four-level active optical clock system based on Rb and Cs frequency standards, respectively. We believe that these findings will aid in overcoming trapping challenges for atomic clocks as well as support studies for physics beyond the standard model.

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