The Implementation of a Compact Cold Atom Interference Gyroscope Based on Miniaturized Quartz Vacuum Chamber

The cold atom interference gyroscope (CAIG) offer substantial potential for rotation measurement due to the high sensitivity and stability. The CAIG with a fountain configuration realized by four-pulse could provide a larger interference-loop area, and enhanced performance. However, this kind of CAI...

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Veröffentlicht in:IEEE sensors journal 2024-01, Vol.24 (24), p.40507-40517
Hauptverfasser: Zhao, Yingpeng, Li, Dianrong, Niu, Jingyu, Bao, Shuning, Zhang, Kaijun, Wang, Yuchen, Cheng, Bing, Zhang, Cheng, Niu, Kexiao, Liu, Yuanzheng, Yue, Yazhou, Wang, Xiaolong, Wu, Bin, Lin, Qiang
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Sprache:eng
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Zusammenfassung:The cold atom interference gyroscope (CAIG) offer substantial potential for rotation measurement due to the high sensitivity and stability. The CAIG with a fountain configuration realized by four-pulse could provide a larger interference-loop area, and enhanced performance. However, this kind of CAIG is usually much larger and higher since it requires a vacuum chamber with sufficient height to achieve a long Raman pulse interval. We demonstrate a four-pulse CAIG based on a miniaturized vacuum chamber that enables portable and transportable rotation rate measurements. The main vacuum chamber is realized by whole glass material. The height of the vacuum unit is 0.7 m, the volume is {{8}.{86} \times {10}^{{4}}}~{{\textrm {cm}}^{{3}}} , and the mass is 75 kg. Then, we estimated the performance of our portable CAIG in the environment of the underground laboratory and the fifth-floor office building. In the laboratory, the sensitivities of the homemade CAIG is {4}.{44}\times {10}^{-{6}} rad/s /(\text {Hz})^{1/2} with an interrogation time of 55 ms and an interference area of 25 mm2. In addition, we measured the angular velocity of the Earth, the relative error is 2.4%. Furthermore, we transported the CAIG to the fifth floor of the office building, which is near the subway. Ultimately, the CAIG achieved a sensitivity of {5}.{47}\times {10}^{-{4}} rad/s /(\text {Hz})^{1/2} . Additionally, the theoretical maximum interrogation time achieved by this CAIG is 124 ms corresponding to a sensitivity of {{5}.{62}\times {10}^{-{8}}}~{/(\text {Hz})^{1/2}} . Our new design of the compact CAIG could provide novel insights into the miniaturization of CAIGs, while also pointing out areas for further improvement.
ISSN:1530-437X
1558-1748
DOI:10.1109/JSEN.2024.3483828