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The design adopts differential configurations for sensing, which eliminates corruption of sensing signals by feedthrough of actuation signal or by thermal drift.
At the circuit level, differential configurations should be used to eliminate all common sources of variations, such as reference electrode drift, solution's pH or ionic strength variations, temperature, or nonspecific binding.
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The differential configuration of the sensor improves signal conditioning and reduces the common-mode noise.
The resulting equations of motion are of coupled ordinary differential configuration, which are usually solved by explicit numerical schemes.
The double differential configuration realizes the temperature self-calibration by making the two pairs of unbalanced masses have the same sensitivity to temperature but opposite sensitivity to acceleration.
The resistance of each heater varies depending on the position of the central stage, with two heaters being used per axis in a differential configuration.
During fatiguing tests surface EMG signals were recorded from biceps brachii muscle with linear arrays of eight electrodes (silver bars 10 mm apart, 5 mm long, and 1 mm diameter) in single differential configuration.
Based on the structure of conventional torsional accelerometers, normally composed of two unbalanced proof masses and an identical torsional beam, this work explores a torsional accelerometer with two structural optimizations aiming to improve the temperature robustness: a double differential configuration and an on-chip integrated reference capacitor configuration.
Comparison tests show that, for most of the accelerometers, by taking the double differential configuration and the on-chip integrated reference capacitor configuration, the temperature sensitivity of the scale factor, the bias stability and the output drift of in the full temperature range are greatly improved.
With restraining a common-mode noise and reducing parasitic couplings, differential configuration is widely used in the LNA circuits.
Second, to reach a quantum-limited sensitivity using an optical phase demodulator in differential configuration.
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