2021
DOI: 10.1016/j.sna.2021.112694
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A sensitive micromachined resonant accelerometer for moving-base gravimetry

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Cited by 36 publications
(10 citation statements)
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“…These results are the best-collected metrics for accelerometers employing the mode-localization paradigm to date, and they are also comparable with state-of-the-art frequency-modulated resonant accelerometers 21 , 46 . Further work on optimizing electronic noise, e.g., the power source noise that contributes to the Lorentzian profile of the resonator via bias and perturbation voltages, can be conducted to approach the ultraprecise level for the application of MEMS gravimeters 47 , 48 . This mode-localized accelerometer is the first to practically display the microseismic background in the frequency interval 0.1–0.5 Hz with a level of 300 ng/√Hz.…”
Section: Discussionmentioning
confidence: 99%
“…These results are the best-collected metrics for accelerometers employing the mode-localization paradigm to date, and they are also comparable with state-of-the-art frequency-modulated resonant accelerometers 21 , 46 . Further work on optimizing electronic noise, e.g., the power source noise that contributes to the Lorentzian profile of the resonator via bias and perturbation voltages, can be conducted to approach the ultraprecise level for the application of MEMS gravimeters 47 , 48 . This mode-localized accelerometer is the first to practically display the microseismic background in the frequency interval 0.1–0.5 Hz with a level of 300 ng/√Hz.…”
Section: Discussionmentioning
confidence: 99%
“…Further miniaturizations and improvements of the MEMS gravimeter, including the implementation of a ceramic vacuum package and a bespoke FPGA board, can result in an increased portability and a reduction in cost, enabling MEMS gravimeters to be used for mineral exploration, geology and other geophysical applications. > REPLACE THIS LINE WITH YOUR MANUSCRIPT ID NUMBER (DOUBLE-CLICK HERE TO EDIT) < Bias Instability [21] 7.35 Hz 18 μGal/√Hz@1 Hz 0.2 mK 8 μGal@~400 s <20 μGal@10-1000 s [22] ~3.1 Hz 8 μGal/√Hz@1 Hz N/A 13.5 μGal@20 s <20 μGal@10-1000 s [24] ~1 kHz 100 μGal/√Hz@1 Hz ±250 μK@ 50℃ 9 μGal@1000 s <50 μGal@10-1000 s [25] kHz 75 ng/√Hz@0.5 Hz ±0.01℃@ 45℃ 17 ng@70 s <30 ng@10-1000 s [40] N/A 10 ng/√Hz@1 Hz ±0.001℃@ 40℃ 7 ng@900 s <40 ng@10-1000 s This work ~14 Hz 1.2 μGal/√Hz@1 Hz 0.4 mK/√Hz@1 mHz 3 μGal@80 s <8 μGal@10-1000 s…”
Section: Discussionmentioning
confidence: 99%
“…A wafer-level vacuum encapsulation of a vibrating beam MEMS accelerometer with a three-stage temperature control was proposed by Mustafazade et al, and recorded the Earth tides and teleseismic events, validating its capability for gravity measurements [24]. More recently, by optimizing the resonator, micro-level and suspension beam structures, a resonant MEMS accelerometer sealed in a hermetic ceramic case within a temperature control chamber was demonstrated by Zheng et al with a bias stability of 0.197 μg/day [25].…”
Section: Introductionmentioning
confidence: 97%
“…Due to the interaction between the geometry nonlinearity (mid-plane stretching) and the force nonlinearity, the curved structure exhibits multiple stable equilibria, snap-through motion and pull-in instabilities along with modal interaction [ 18 , 19 , 20 , 21 , 22 ]. It is well acknowledged that there are abundant nonlinear phenomena in MEMS while extending the micro-devices driving forces into the nonlinear regimes [ 23 , 24 , 25 , 26 , 27 , 28 , 29 , 30 , 31 ]. Essentially, a large excitation will significantly increase the vibration amplitude and thus improve the performance of such devices [ 32 , 33 , 34 ].…”
Section: Introductionmentioning
confidence: 99%