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8.2 Micromachined Accelerometer                                               189

                  alignment to the sense axes, as the sensing elements are defined by highly accurate
                  photolithographic methods. Three-axis sensors with piezoresistive, piezoelectric,
                  and capacitive position sensing mechanisms have been reported. Two approaches
                  are possible: a single proof mass that is compliant to move along two or even three
                  axes, or several proof masses integrated on one chip for the different sense axes.
                  Cross-axis sensitivity is a major issue with multiaxis accelerometers.
                      An interesting prototype has been reported by Lemkin et al. [42]. It uses a
                  surface-micromachined single proof mass, which is compliant to movement along
                  all three axes, as shown in Figure 8.14. The 2.3-µm-thick sensing element has inter-
                  digitated comb fingers on all four sides so that acceleration can be sensed in the two
                  in-plane axes. The sensing element is designed with a common centroid layout;
                  hence, both translational and rotational off-axis accelerations become a common
                  mode signal, which is rejected to the first order by the differential signal pick-off. It
                  is also compliant to movements out of plane, which changes the air-gap of a capaci-
                  tor formed by an electrode under the proof mass and the center section of the proof
                  mass. The pick-off circuit in this direction is quasidifferential as it is referenced to a
                  fixed capacitor, which is formed by a separate mechanical structure.
                      Figure 8.15 shows the front-end of the pick-off circuit. The proof mass, which
                  acts as the common node center node to all three capacitive half-bridges, is driven
                  with a step voltage, and the adjacent fixed electrodes are connected to a differential
                  charge amplifier. The output voltage is proportional to the differential change in
                  capacitance. Subsequently, this voltage is sampled and held, as the same capacitors
                  are then used as electrostatic actuators. Feedback voltage pulses are applied to the
                  electrode further away from the proof mass, forcing it to the nominal center posi-
                  tion. The force-balancing system relies again on the incorporation of the proof mass
                  in a sigma-delta modulator type control system, one for each sensing axes. The
                  reported noise floor is about 0.73 mG/√Hz for all three axes. Especially impressive
                  is the low cross-axis sensitivity of below 1%, which is better than many commercial
                  grade single-axis devices.
                      The same authors developed a prototype with three separate proof masses on
                  the same chip but using the same technology and interface and control strategy [43].
                  The performance for this sensor was improved, compared to that of the single-mass
                  sensor, showing a measured noise floor of 160 mG/√Hz for x- and y-axes and 990
                  mG/√Hz for z-axis. This corresponds to a dynamic range of 84, 81, and 70 dB for





















                  Figure 8.14  Sensing element of a three-axis capacitive accelerometer.
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