Publication | Closed Access
Lasing of cesium active optical clock with 459 nm laser pumping
18
Citations
15
References
2014
Year
Unknown Venue
Optical MaterialsEngineeringLaser ScienceLaser ApplicationsLaser PhysicsLaser MaterialSuper-intense LasersHigh-power LasersLaser TechnologyOptical PropertiesCs Cell TemperatureLaser CommunicationsOptical PumpingPhotonicsLaser PumpingPhysicsLaser DesignLaser CompositionCavity BandwidthElectro-optics DeviceApplied PhysicsActive Optical ClockOptoelectronics
We realize the lasing of cesium active optical clock with 459 nm laser pumping, which operates deep in the optical bad-cavity regime. The ratio between cavity bandwidth and gain bandwidth is 55.08 theoretically. With 459 nm laser pumping, the population inversion occurs between the cesium 7S <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1/2</inf> state and 6P <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3/2</inf> state, and the stimulated radiation between the two states is realized. The 1469.9 nm output signal of cesium active optical clock can reach a power of 8 μW. The output power also shows a threshold character with pumping laser power and can be influenced by the Cs cell temperature. This active optical clock has an advantage in stability over the conventional optical clocks, due to its suppression of cavity pulling effect, which is also demonstrated experimentally.
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