Cesium based laser-atomic oscillator

We report the first demonstration of a laser-atomic oscillator with cesium (Cs) atoms. A laser-atomic oscillator is analogous to an active mode-locked laser with a self-excited modulator, i.e., atoms, at a ground-state hyperfine transition frequency. Therefore, a laser-atomic oscillator can be configured as the simplest active atomic clock or a self-oscillating, earth-field atomic magnetometer that delivers oscillation signals both optically and electrically. With the current experimental Cs laser-atomic oscillator (Cs-LAO) setup, when it is configured as an atomic clock using the 0–0 hyperfine transition, the short-term fractional frequency instability is around the 10−10 level. When it is configured as a self-oscillating magnetometer using a magnetically sensitive 3–3 hyperfine transition, the magnetic field sensitivity is around 100 fT/Hz at 60 Hz. The presented Cs-LAO uses a cavity length from ∼6.5 to ∼11.4 cm. Ultimately, the minimal length of a Cs-LAO device can be ≤1.63 cm. Our new efforts unlock the potential of building truly chip-scale atomic clocks and magnetometers.

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Publication Details

Journal
Applied Physics Letters
Published
2026-10-26
DOI
https://doi.org/10.1063/5.0351892
Primary Topic
Advanced Frequency and Time Standards
Type
article
Field-Weighted Citation Impact
0.00

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article

Cesium based laser-atomic oscillator

Yuan‐Yu Jau, Roger Ding, George R. Burns, Saurabh Pandey
Applied Physics Letters
Advanced Frequency and Time Standards
article

Cesium based laser-atomic oscillator

Yuan‐Yu Jau, Roger Ding, George R. Burns, Saurabh Pandey
article en

Abstract

We report the first demonstration of a laser-atomic oscillator with cesium (Cs) atoms. A laser-atomic oscillator is analogous to an active mode-locked laser with a self-excited modulator, i.e., atoms, at a ground-state hyperfine transition frequency. Therefore, a laser-atomic oscillator can be configured as the simplest active atomic clock or a self-oscillating, earth-field atomic magnetometer that delivers oscillation signals both optically and electrically. With the current experimental Cs laser-atomic oscillator (Cs-LAO) setup, when it is configured as an atomic clock using the 0–0 hyperfine transition, the short-term fractional frequency instability is around the 10−10 level. When it is configured as a self-oscillating magnetometer using a magnetically sensitive 3–3 hyperfine transition, the magnetic field sensitivity is around 100 fT/Hz at 60 Hz. The presented Cs-LAO uses a cavity length from ∼6.5 to ∼11.4 cm. Ultimately, the minimal length of a Cs-LAO device can be ≤1.63 cm. Our new efforts unlock the potential of building truly chip-scale atomic clocks and magnetometers.

Applied Physics LettersVol. 129(17)
Sandia National Laboratories (US)
U.S. Department of Energy, Defense Advanced Research Projects Agency, National Nuclear Security Administration, Sandia National Laboratories
Openalex Percentile: Top 55%
Advanced Frequency and Time Standards
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Cesium based laser-atomic oscillator — Yuan‐Yu Jau, Roger Ding, et al. · Applied Physics Letters (2026) | TGRS Research Map | TGRS