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PreprintCC BY 4.0arXiv

Cesium Based Laser-Atomic Oscillator

Abstract

We report the first demonstration of a laser-atomic oscillator with cesium (Cs) atoms. A laser-atomic oscillator (LAO) 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 LAO 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-LAO setup, when it is configured as an atomic clock using the 0--0 hyperfine transition, the short-term fractional frequency instability is around 10−10 level. When it is configured as a self-oscillating magnetometer using a magnetically-sensitive 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 cm 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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BibTeX
@misc{pandey2026cesium,
  title = {{Cesium Based Laser-Atomic Oscillator}},
  author = {Saurabh Pandey and Roger Ding and George Burns and Yuan-Yu Jau},
  howpublished = {arXiv},
  year = {2026},
  month = jun,
  doi = {10.48550/arxiv.2606.32019},
  eprint = {2606.32019},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2606.32019},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Cesium Based Laser-Atomic Oscillator
AU  - Saurabh Pandey
AU  - Roger Ding
AU  - George Burns
AU  - Yuan-Yu Jau
PY  - 2026
DA  - 2026/06/30
PB  - arXiv
DO  - 10.48550/arxiv.2606.32019
UR  - https://arxiv.org/abs/2606.32019
AB  - We report the first demonstration of a laser-atomic oscillator with cesium (Cs) atoms. A laser-atomic oscillator (LAO) 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 LAO 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-LAO setup, when it is configured as an atomic clock using the 0--0 hyperfine transition, the short-term fractional frequency instability is around 10^−10 level. When it is configured as a self-oscillating magnetometer using a magnetically-sensitive 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 cm 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.
ER  -