First demonstration of a cesium laser-atomic oscillator achieving ~10^{-10} fractional frequency instability as a clock and ~100 fT/sqrt(Hz) sensitivity as a magnetometer, with cavity lengths allowing potential miniaturization to ≤1.63 cm.
Temperature and pressure shift of the Cs clock transition in the presence of buffer gases: Ne,
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physics.atom-ph 2years
2026 2verdicts
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Asymmetry in bichromatic fields produces additional nonlinear error-signal frequency shifts in CPT spectroscopy at phase-jump modulation under unisotropic relaxation, while conventional harmonic modulation yields more linear shifts in the high-frequency regime for non-short integration times.
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Cesium Based Laser-Atomic Oscillator
First demonstration of a cesium laser-atomic oscillator achieving ~10^{-10} fractional frequency instability as a clock and ~100 fT/sqrt(Hz) sensitivity as a magnetometer, with cavity lengths allowing potential miniaturization to ≤1.63 cm.
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Analysis of the frequency shift in coherent population trapping resonance's dynamic continuous-wave spectroscopy at the phase-jump modulation and its comparison with the conventional approach
Asymmetry in bichromatic fields produces additional nonlinear error-signal frequency shifts in CPT spectroscopy at phase-jump modulation under unisotropic relaxation, while conventional harmonic modulation yields more linear shifts in the high-frequency regime for non-short integration times.