scholarly journals Dependence of sensitivity of atom interferometer gravimeters on the Raman laser pulse sequences

2009 ◽  
Vol 58 (12) ◽  
pp. 8230
Author(s):  
Ren Li-Chun ◽  
Zhou Lin ◽  
Li Run-Bing ◽  
Liu Min ◽  
Wang Jin ◽  
...  
2014 ◽  
Vol 68 (11) ◽  
Author(s):  
Bing Cheng ◽  
Zhaoying Wang ◽  
Bin Wu ◽  
Aopeng Xu ◽  
Qiyu Wang ◽  
...  

1986 ◽  
Vol 64 (6) ◽  
pp. 743-745
Author(s):  
R. Marchand ◽  
R. Fedosejevs ◽  
I. V. Tomov

Quenching of the forward Stokes by phase matching in a Raman-active medium is revisited. A parameter range is identified where the small signal gain of the forward Stokes is a decreasing function of the pump intensity. The relevance of this effect to the reduction of the troublesome second Stokes in a Raman laser-pulse compressor is also discussed.


Photonics ◽  
2020 ◽  
Vol 7 (2) ◽  
pp. 32
Author(s):  
Yang Zhao ◽  
Shaokai Wang ◽  
Wei Zhuang ◽  
Tianchu Li

The paper describes a Raman-laser system with high performance for an absolute gravimeter that was based on 87Rb atom interferometer. As our gravimeter is a part of the standard acceleration of gravity of China, the Raman lasers’ characteristics should be considered. This laser system includes two diode lasers. The master laser is frequency locked through the frequency-modulation (FM) spectroscopy technology. Its maximum frequency drift is better than 50 kHz in 11 h, which is measured by home-made optical frequency comb. The slave laser is phase locked to the master laser with a frequency difference of 6.8346 GHz while using an optical phase lock loop (OPLL). The phase noise is lower than −105 dBc/Hz at the Fourier frequency from 200 Hz to 42 kHz. It is limited by the measurement sensitivity of the signal source analyzer in low Fourier frequency. Furthermore, the power fluctuation of Raman lasers’ pulses is also suppressed by a fast power servo system. While using this servo system, Raman lasers’ pulses could be fast re-locked while its fast turning on again in the pulse sequence. The peak value fluctuation of the laser power pulses is decreased from 25% to 0.7%, which is improved over 35 times. This Raman-laser system can stably operate over 500 h, which is suited for long-term highly precise and accurate gravity measurements.


2017 ◽  
Vol 66 (21) ◽  
pp. 213301
Author(s):  
Zhang Lu ◽  
Yan Lu-Yao ◽  
Bao Hui-Han ◽  
Chai Xiao-Qian ◽  
Ma Dan-Dan ◽  
...  

2012 ◽  
Vol 531 ◽  
pp. 185-188
Author(s):  
Cong Wang ◽  
Xing Yu Zhang ◽  
Qing Pu Wang ◽  
Xiao Han Chen ◽  
Zhen Hua Cong ◽  
...  

We consider a bulk silicon crystal as a Mid-IR Raman amplifier and study its Raman amplification. A Raman amplifier is established when an intense pump laser pulse and a Raman laser pulse pass through one silicon simultaneously, with good spatial and temporal overlap. Considering the situation of pumping wavelength at 2.94 μm achievable by using an Er:YAG laser and Raman laser wavelength at 3.47 μm with the 521 cm-1 Raman shift, the properties of the output amplified Raman laser are investigated by numerically solving the coupled transfer equations.


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