Chinese Journal of Lasers, Volume. 45, Issue 9, 901001(2018)
Ultra-Stable Cavity System with Low Drift Rate for Mercury Optical Lattice Clock
Fig. 2. Schematics of temperature stabilizer circuit. (a) Schematic of temperature collection and amplification circuit; (b) schematic of PID control circuit
Fig. 4. Variation of measured resonant frequency or calculated resonant frequency with time
Fig. 5. (a) Temperature at different positions of active temperature stabilized layer; (b) environmental temperature of laboratory
Fig. 6. Temperature noise power spectrum density of three measuring points in the active temperature stabilized layer (solid line), temperature noise power spectrum density of three measuring points in the ultra-stable cavity (dotted line) calculated by transfer function, and the requirement of the temperature noise power spectrum density at 10-8 K-1and 10-9 K-1 to reach the thermal noise limit
Fig. 7. (a) Temperature fluctuation of the ultra-stable cavity which calculated from the temperature of temperature stabilized layer; (b) temperature stability of the three point (middle, top, bottom) in stabilized layer (solid points), temperature stability of the ultra-stable cavity (hollow points) calculated from the temperature of the stabilized layer, and the requirement of the temperature stability at 10-8 K-1 and 10-9 K-1(brown line and green line) to reach the thermal noise limit
Fig. 8. Experimental schematic of the clock transition detection of 199Hg cold atoms
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Fu Xiaohu, Fang Su, Zhao Ruchen, Sun Jianfang, Zhang Ye, Xu Zhen, Wang Yuzhu. Ultra-Stable Cavity System with Low Drift Rate for Mercury Optical Lattice Clock[J]. Chinese Journal of Lasers, 2018, 45(9): 901001
Category: laser devices and laser physics
Received: Feb. 21, 2018
Accepted: --
Published Online: Sep. 8, 2018
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