Author Affiliations
MOE Key Laboratory of Fundamental Physical Quantities Measurement & Hubei Key Laboratory of Gravitation and Quantum Physics, PGMF and School of Physics, Huazhong University of Science and Technology, Wuhan 430074, Chinashow less
Fig. 1. (a) Stimulated Raman transition in three-level system and (b) momentum transfer in stimulated Raman transition.
Fig. 2. Structure of Mach–Zender-type atom interferometry.
Fig. 3. Typical process of atom interferometer with parabolic trajectory.
Fig. 4. (a) Polarization configurations in a hollow pyramidal MOT. (b) MOT array in Imperial College London. (c) Experiment setup of pyramidal atom gravimeter using single laser beam in LNE-SYRTE. Panel (a) reprinted with permission from Ref. [59] of the Optical Society. Panel (b) reprinted with permission from Ref. [60] of the Optical Society. Panel (c) reprinted from Ref. [61], with the permission of AIP Publishing.
Fig. 5. Atom chips reported by (a) University of Innsbruck and (b) University of Strathclyde. Panel (a) reprinted with permission from Ref. [65] Copyright (2000) by the American Physical Society. Panel (b) reprinted by permission from Ref. [67] Copyright (2013) by the Springer Nature.
Fig. 6. Fiber optical system using single laser source based on telecom C-band.
Fig. 7. (A) Measurement route, (B) gravity anomaly as a function of the elevation. (C) Atomic gravimeter inside a vehicle. (D) The atomic gravimeter apparatus. Reprinted by permission from Ref. [42]. Copyright (2019) by the AAAS. (© The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC) http://creativecommons.org/licenses/by-nc/4.0/).
Fig. 8. Picture of cold atom gravimeter installed on a gyro-stabilized platform next to a spring gravimeter. Reprinted by permission from Ref. [76]. Copyright (2018) by the Springer Nature.
Fig. 9. (a) Flight plan of Iceland gravity campaign. (b) Comparison between airborne measurements and ground measurements upward continued. Reprinted by permission from Ref. [84]. Copyright (2020) by the Springer Nature.
Fig. 10. (a) Acceleration signal recorded by the MAs. (b) AI discrete measurements. Corresponding to the atomic fluorescence of the 87Rb atoms in the F = 2 state, normalized to the fluorescence of all the atoms. (c) and (d) Atomic measurements plotted versus the signal stemming from the MAs at 1 g (c) and 0 g (d). Reprinted by permission from Ref. [87]. Copyright (2011) by the Springer Nature.
Fig. 11. Mach–Zehnder interferometry of a BEC in microgravity as realized in the ZARM drop tower in Bremen (a), where absorption imaging (b) brings out the interference fringes (c). Reprinted with permission from Ref. [99]. Copyright (2013) by the American Physical Society.
Group | T/ms | Sensitivity/() | Uncertainty/μGal | Ref. |
---|
SYRTE | 80 | 5.7 | 4.3 | [39,40] | Stanford Uni. | 400 | 8 | 3.4 | [29,41] | Humboldt Uni. | 260 | 9.6 | 3.2 | [31] | Berkeley | 130 | 37 | 15 | [42] | ONERA | 48 | 42 | 25 | [43] | HUST | 300 | 4.2 | 3.0 | [34,44] | WIPM | 200 | 28 | 9.0 | [45,46] | NIM | 70 | 44 | 5.2 | [47] | ZJUT | 60 | 90 | 19 | [48] |
|
Table 1. State-of-the-art in gravimeters based on stimulated Raman transition (1 μGal = 10−8 m/s2).