Patent Description:
Accelerometers function by detecting a displacement of a proof mass under inertial forces. In one example, an accelerometer may detect the displacement of a proof mass by the change in frequency of a resonator connected between the proof mass and a support base. A resonator, which may be designed to change frequency proportional to the load applied to the resonator by the proof mass under acceleration. The resonator may be electrically coupled to an oscillator, or other signal generation circuit, which causes the resonator to vibrate at its resonant frequency.

<CIT> discloses a resonant sensor comprising: a substrate; a proof mass suspended from the substrate to allow for relative movement between the proof mass and the substrate along at least one sensitive axis; at least one resonant element coupled to the proof mass; and an electrode assembly adjacent to the at least one resonant element.

<CIT> discloses a silicon micro-resonance type accelerometer and a self-testing method thereof. The silicon micro-resonance type accelerometer comprises a resonator, a mass block and a self-testing structure.

<CIT> discloses an integrated circuit die includes a microelectromechanical system (MEMS) device formed using a MEMS structural layer of the integrated circuit die. The integrated circuit die includes a monitor structure configured to generate an indicator of a device parameter of the MEMS device. The monitor structure may include a partitioned electrode of the MEMS device.

Systems and techniques for measurement of proof mass motion at wafer-level probe testing prior to packaging are described. In some examples, a built-in test actuator of a microelectromechanical system (MEMS) vibrating beam accelerometer (VBA) is disclosed.

The disclosure is directed to a MEMS VBA including one or more built-in test actuators. VBAs function by using a proof mass to apply inertial force to one or more vibrating beams, or resonators, such that the applied acceleration can be measured as a change in resonant frequency of the vibrating beam(s). Control electronics interface with resonator drive and sense electrodes to sustain motion of the vibrating beam(s). Typically, two vibrating beams are arranged with opposing scale factors, in hertz/g (Hz/g, where g represents acceleration due to gravity near the surface of the earth), so that the differential frequency (f<NUM> - f<NUM>) represents measured acceleration. This differential frequency output helps reject common-mode error sources, as described further below.

In some examples, including one or more built-in test actuators enables measurement of proof mass motion at wafer-level probe testing so that failing devices can be screened out earlier in the manufacturing process, e.g., prior to packaging. Typically, wafer-level probe testing only verifies that the two resonators are functioning normally. Usually, one cannot shake or tilt the wafer-level probe tester to induce motion of the proof mass. Failures associated with proof mass motion, such as broken flexures or stuck devices, can then only be detected by visual inspection or after packaging when the device can be tumbled, for example, between +/- <NUM>, where g denotes an acceleration equal to an acceleration caused by gravity at or near the surface of Earth.

In some examples, measurement of proof mass motion via one or more built-in test actuators may enable a better characterization of the quality factor (Q) associated with the proof mass natural frequency. For example, Q is difficult to measure accurately on a shaker since fixturing needed for typical test setups often adds unexpected mechanical resonances (with frequencies on the order of kHz), whereas such mechanical resonances are not present when measuring Q via built-in test actuators.

<FIG> is a conceptual diagram illustrating a MEMS VBA with X-direction resonators and proof mass actuator electrodes. <FIG> is a top view of MEMS VBA <NUM> showing the anchor <NUM> to the support base, but the support base is not shown.

MEMS VBA <NUM> includes pendulous proof mass <NUM> connected to a rigid resonator connection structure <NUM> at hinge flexure <NUM>, and resonators 18A and 18B. For a pendulous MEMS VBA according to this disclosure, proof mass <NUM> may move in a plane parallel to the plane of the support base (not shown in <FIG>). A support base may be a substrate of, for example, a glass or silicon wafer. Resonators 18A and 18B of MEMS VBA <NUM> convert the inertial force of proof mass <NUM> under acceleration, to a change in the driven resonant frequency. The MEMS VBA outputs a change in the resonant frequency of each resonator as an indication of the amount of acceleration. In some examples, the resonators may be located adjacent to the proof mass so that the resonators receive the proof mass force amplified through lever action. Although the example shown in <FIG> includes two resonators, in some examples MEMS VBA <NUM> may include fewer or more resonators, e.g., one resonator or three or more resonators.

MEMS VBA <NUM> may be fabricated from a dissolved wafer process that produces MEMS VBA <NUM> as a silicon mechanical structure tethered to lower and upper glass substrates (not shown in <FIG>) at specific anchor regions, e.g. anchor <NUM>. The glass substrates may be etched in other areas to define released regions of MEMS VBA <NUM>, which include air gaps that allow the silicon portions, such as proof mass <NUM>, to move freely relative to the substrate. Areas which are not etched are bonded to silicon to define mechanical anchors. The geometry of both the silicon mechanism and anchor regions may be defined by photolithography.

A dissolved wafer process to fabricate a silicon MEMS VBA and glass substrates is just one example of a technique to fabricate a MEMS VBA of this disclosure. Other techniques may be used to fabricate the geometry of MEMS VBA <NUM>. Some other examples may include materials such as quartz (SiO2), piezoelectric material and similar materials. Other processes may include isotropic etching, chemical etching, deep reactive-ion etching (DRIE) and similar processes. In the example of <FIG>, proof mass <NUM>, resonator connection structure <NUM>, hinge flexure <NUM>, resonators 18A, 18B may be comprised of a monolithic material, which results in the components of MEMS VBA <NUM> all with the same coefficient of thermal expansion (CTE). The components of MEMS VBA <NUM> are all in the same plane, parallel to the X-Y plane as shown in <FIG>.

Proof mass <NUM> connects to resonator connection structure <NUM> at anchor <NUM> by hinge flexure <NUM>. The point at which hinge flexure <NUM> connects to anchor <NUM> is the center of rotation for proof mass <NUM>. Left and right resonators 18A and 18B connect to the same primary anchor <NUM> by rigid resonator connection structure <NUM>. Resonators 18A and 18B connect to proof mass <NUM> at a distance r<NUM> from the center of rotation for proof mass <NUM>. Center of mass <NUM> for proof mass <NUM> is at a distance r<NUM> from the center of rotation for proof mass <NUM>. This results in the inertial force of proof mass <NUM> amplified by the leverage ratio r<NUM>/r<NUM>.

In other words, hinge flexure <NUM> may be configured to flexibly connect proof mass <NUM> to the resonator connection structure <NUM>. Hinge flexure <NUM> suspends proof mass <NUM> parallel to the support base (not shown in <FIG>) at anchor <NUM>. In response to an acceleration of MEMS VBA <NUM>, proof mass <NUM> rotates about the hinge flexure <NUM> in its plane, parallel to the X-Y plane and parallel to the plane of the support base (not shown in <FIG>). The support base of this disclosure may be formed from the substrate using the etching processes described above.

Resonators 18A and 18B, in the example of <FIG>, include anchored combs and resonator beams with released combs. Resonator 18A includes resonator beam 19A with released combs and anchored combs 26A - 26C and resonator 18B includes resonator beam 19B with released combs and anchored combs 20A - 20C. In some examples, anchored combs may be referred to as stator combs. Resonators 18A and 18B are configured to flexibly connect the pendulous proof mass <NUM> to resonator connection structure <NUM> with resonator beams 19A and 19B and to flex within the plane of proof mass <NUM> based on the rotation of the proof mass <NUM> about hinge flexure <NUM>.

Each of the two resonators 18A and 18B resonate at a respective resonant frequency, which, in some examples may be approximately the same frequency. MEMS VBA <NUM> includes metal layers deposited onto the glass substrates (not shown in <FIG>). These metal layers define electrical wires that connect silicon electrodes to bond pads. The bond pads may be external to MEMS VBA <NUM> and used to electrically connect to external circuitry that excites and sustains mechanical motion at the resonant frequency for each resonator 18A and 18B through electrostatic actuation, e.g. by applying an electric charge. In the presence of external acceleration, proof mass <NUM> will deflect and apply axial force to resonator beams 19A and 19B of resonators 18A and 18B. This axial force from proof mass <NUM> causes a change in the driven resonant frequency such that the frequency change may be used to measure external acceleration on MEMS VBA <NUM>.

The tines of the released combs on resonator beams 19A - 19B and anchored combs 20A - 20C and 26A - 26C may enable detection of the change in resonant frequency, which may be translated as an amount of force (e.g., increase or decrease of force) and further translated as the amount of acceleration on MEMS VBA <NUM>. For example, during calibration, the change in frequency may be mapped to a force on the resonator beam, which may be further mapped to an amount of acceleration on MEMS VBA <NUM>. In the example of <FIG>, the two resonators 18A and 18B allow for a differential frequency measurement results from change in frequency when a force (e.g., compression or tension) is placed on the two resonator beams 19A - 19B by rotation of proof mass <NUM>.

The differential frequency measurement output by the sense signals from MEMS VBA <NUM> is used to reject sources of error common to both resonators. One example may include a temperature change. That is, a change in operating condition, such as a temperature change may affect both resonators the same way. A second example would be any shift in voltages applied to both resonators. A differential frequency measurement may subtract sources of common error applied to both resonators by subtracting the common error and leaving approximately just the signal caused by acceleration on MEMS VBA <NUM>. The differential frequency measurement may then ultimately lead to improved bias repeatability for the accelerometer.

In some examples, the resonators may have a different resonant frequency, for example, resonator 18A may be configured to resonate at a different frequency than resonator 18B. In some examples, the mass of one resonator may be configured to be different from one or more other resonators. A MEMS VBA with resonators that have a different resonant frequency may provide a benefit, for example, when the MEMS VBA is at zero g, (e.g., substantially no acceleration experienced by the MEMS VBA) the resonators may not vibrate at exactly the same frequency. The different frequency at zero g causes an intentional offset in the MEMS VBA and may result in improved detectability and performance.

In the example of <FIG>, two resonators are used to provide a differential frequency measurement. In other examples, the techniques of this disclosure may also apply to MEMS VBA's with more or fewer resonators. In other examples, the one or more resonators may be oriented at any angle, not just x and y while still using the techniques of this disclosure. Though shown as double-ended tuning fork (DETF) comb resonators in the example of <FIG>, in other examples, resonators 18A and 18B may be configured as other types of resonators. For example, instead of DETF, resonators 18A and 18B may be single resonator beam or a more complex resonator geometry. Also, resonator beams 19A and 1B may comprise a piezoelectric material and may not include comb tines.

In the example of MEMS VBA <NUM>, resonators 18A - 18B are configured to flex in a direction substantially parallel to a long axis of the resonator connection structure <NUM>. The long axis of resonator connection structure <NUM> is parallel to the X-axis in the example of <FIG>. Resonators 18A - 18B are oriented along the X-axis in the example of MEMS VBA <NUM>. In this disclosure, substantially parallel means structures or planes are parallel within manufacturing and measurement tolerances.

Resonator connection structure <NUM> connects resonators 18A - 18B to primary anchor <NUM> through a sufficiently rigid connection that allows proof mass <NUM> to exert axial force on the resonator beams. Resonator connection structure <NUM> is sized to be stiffer than the axial spring constant of the resonators. The geometry of resonator connection structure <NUM> and resonators 18A - 18B, according to the techniques of this disclosure, configure proof mass <NUM>, resonator beams 19A - 19B and resonator connection structure <NUM> to be connected to the support base by the single region at anchor <NUM>. Resonator connection structure <NUM> may reduce or prevent bias errors that may otherwise result from the thermal expansion mismatch between the glass substrate (support base) and the silicon mechanism (e.g., pendulous proof mass <NUM>). In other words, the design of the silicon and glass masks are such that both the proof mass <NUM> and resonators 18A - 18B are primarily anchored to a single region, e.g., at anchor <NUM>.

An advantage of the geometry of a MEMS VBA of this disclosure may include reducing or preventing thermal expansion mismatch, as well as other forces exerted on the substrate from reaching resonators 18A - 18B and significantly straining the resonator beams. The geometry of this disclosure may have an advantage of ultimately providing a more precise measurement of external acceleration when compared to a MEMS VBA with different geometry. In other words, anchor <NUM> may be configured to allow a first thermal expansion of the support base, and a second thermal expansion of the monolithic material of resonators 18A - 18B and resonator connection structure <NUM>, in examples in which the first thermal expansion is different than the second thermal expansion. The geometry of resonator connection structure <NUM> is configured to substantially prevent other forces applied to the support base from transferring to either the pendulous proof mass <NUM> or the at least two resonators. Some examples of other forces may include forces applied to MEMS VBA <NUM> by the circuit board, or other structure, on which MEMS VBA <NUM> is mounted. The circuit board may be subjected to forces, such as squeezing or twisting that may be transferred to the components on the circuit board, including MEMS VBA <NUM>.

In the example of <FIG>, MEMS VBA <NUM> may be fabricated as one of a plurality of MEMS VBAs <NUM> on a wafer (not shown). The wafer may include proof mass actuator electrodes 30A and 30B. In some examples, proof mass actuator electrodes 30A and 30B may be included with MEMS VBA <NUM>. In some examples, the wafer and/or MEMS VBA <NUM> may include one proof mass actuator electrode, e.g., one or either proof mass actuator 30A or 30B. In some examples, the wafer and/or MEMS VBA <NUM> may include more than two proof mass actuator electrodes, e.g., three or more proof mass actuator electrodes. Proof mass actuator electrodes 30A and 30B may be silicon electrodes connected to bond pads, such as those described above, which may be connected to external circuitry that excites mechanical motion at one or more predetermined frequencies of proof mass <NUM> through electrostatic actuation, e.g., by applying an electric charge, a current signal, and/or a voltage signal to proof mass actuator electrodes 30A and 30B. In the example shown, there is a small air gap between each proof mass actuator electrode 30A and 30B and proof mass <NUM>. Proof mass actuator electrodes 30A and 30B may be configured as parallel-plate electrodes causing a displacement (dx) of proof mass <NUM> in response to a capacitance change (ΔC) of proof mass actuator electrodes 30A and 30B. In some examples, proof mass actuator electrodes 30A and 30B may be configured to displace proof mass <NUM> by a predetermined distance.

In some examples, one or the other of proof mass actuator electrodes 30A and 30B may be configured to drive proof mass <NUM>, and the other of proof mass actuator electrodes 30A and 30B may be configured to sense the motion of proof mass <NUM> and may be connected to read-out a signal circuitry. In some examples, one proof mass actuator electrode, either 30A or 30B, may be configured to drive proof mass <NUM> and sense the motion of proof mass <NUM>, and may be connected to read-out circuitry. In some examples, both proof mass actuator electrodes 30A and 30B may be configured to drive proof mass <NUM> and one or both of resonators 18A and 18B may be configured to sense the motion of proof mass <NUM> and may be connected to read-out circuitry.

In some examples, resonator electrodes (not shown) may be configured to drive resonators 18A and 18B in closed loop oscillation. A direct current (DC) or slowly varying voltage signal may be applied to each proof mass actuator electrode 30A and 30B to create electrostatic force, and the frequency change of resonators 18A and 18B may be observed to assess scale factor in Hz/g. Driving resonators 18A and 18B in closed loop oscillation and observing the frequency change of resonators 18A and 18B may enable verification that proof mass <NUM> is correctly connected to resonators 18A and 18B to cause the expected frequency shifts.

In some examples, one or more proof mass actuator electrodes 30A and 30B may be configured as comb fingers having a linear capacitance versus displacement relationship. In some examples, proof mass actuator electrodes 30A and 30B may be embedded within proof mass <NUM>. Although two proof mass actuator electrodes are shown, more or fewer proof mass actuator electrodes may be included and/or used. In some examples, after interim testing using proof mass actuator electrodes 30A and 30B has been completed, e.g., during wafer-level probe testing and package testing, a circuit board (not shown) controlling resonators 18A and 18B may connect proof mass actuator electrodes 30A and 30B to ground, e.g., such that only inertial forces are acting upon proof mass <NUM> when in use.

<FIG> is a functional block diagram illustrating a system <NUM> including a MEMS VBA <NUM>, according to one or more techniques of this disclosure. The functional blocks of system <NUM> are just one example of a system that may include a MEMS VBA according to this disclosure. In other examples, functional blocks may be combined, or functions may be grouped in a different manner than depicted in <FIG>. In some examples, any or all of the functional blocks illustrated and described with respect to <FIG> may be included with MEMS VBA <NUM>, e.g., any or all of the functional blocks may be a part of MEMS VBA <NUM>. Other circuitry <NUM> may include power supply circuits and other processing circuits that may use the output of MEMS VBA <NUM> to perform various functions, e.g. inertial navigation and motion sensing.

System <NUM> may include processing circuitry <NUM>, resonator driver circuits 104A and 104B, proof mass actuator electrode driver circuits 114A and 114B, and MEMS VBA <NUM>. MEMS VBA <NUM> may include any VBA, including the pendulous proof mass MEMS VBAs described above in relation to <FIG>.

In the example of <FIG>, resonator driver circuits 104A and 104B are operatively connected to MEMS VBA <NUM> and may send resonator drive signals 106A and 106B to MEMS VBA <NUM> as well as receive resonator sense signals 108A and 108B from MEMS VBA <NUM>. In the example of <FIG>, resonator driver circuit 104A may be coupled to one resonator, e.g., resonator 18A depicted in <FIG>, and resonator driver circuit 104B may be coupled to a second resonator, e.g. resonator 18B. Resonator driver circuits 104A and 104B may be configured to output a signal that causes the resonators of MEMS VBA <NUM> to vibrate at a respective resonant frequency of each of the resonators. In some examples, vibrate means to excite and sustain mechanical motion for each resonator through electrostatic actuation. In some examples, resonator driver circuits 104A and 104B may include one or more oscillator circuits. In some examples the signal to MEMS VBA <NUM> may travel along conductive pathways along or within a support base of accelerometer. The signal from resonator driver circuits 104A and 104B may provide a patterned electric field to cause resonators of MEMS VBA <NUM> to maintain resonance.

Resonator driver circuit 104A may output drive signal 106A at a different frequency than drive signal 106B from resonator driver circuit 104B. The example of <FIG> may be configured to determine a differential frequency signal based on resonator sense signals 108A and 108B. Resonator driver circuits 104A and 104B may adjust the output of resonator drive signals 106A and 106B based on the feedback loop from resonator sense signals 108A and 108B, e.g., to maintain the resonators at the respective resonant frequency. As described above, a MEMS VBA according to this disclosure may include one resonator or more than two resonators and may also include fewer or additional resonator driver circuits.

As described above in relation to <FIG>, an acceleration of the pendulous mass MEMS VBA, e.g., in a direction substantially parallel to the plane of the proof mass, may cause a rotation of the pendulous proof mass about the hinge flexure parallel to the plane of the proof mass. The resonators of MEMS VBA <NUM> may be configured to receive a force, in response to the rotation of the proof mass, such that the force causes a respective change in resonant frequency of at least one resonator.

Processing circuitry <NUM> may communicate with resonator driver circuits 104A and 104B. Processing circuitry <NUM> may include various signal processing functions, such as filtering, amplification and analog-to-digital conversion (ADC). Filtering functions may include high-pass, band-pass, or other types of signal filtering. In some examples, resonator driver circuits 104A and 104B may also include signal processing functions, such as amplification and filtering. Processing circuitry <NUM> may output the processed signal received from MEMS VBA <NUM> to other circuitry <NUM> as an analog or digital signal. Processing circuitry <NUM> may also receive signals from other circuitry <NUM>, such as command signals, calibration signals and similar signals.

Processing circuitry <NUM> may operatively connect to MEMS VBA <NUM> , e.g., via resonator driver circuits 104A and 104B. Processing circuitry <NUM> may be configured to receive the signal from MEMS VBA <NUM>, which may indicate of a respective change in the resonant frequency of at least one resonator of MEMS VBA <NUM>. Based on the respective change in resonant frequency, processing circuitry <NUM> may determine an acceleration measurement, or otherwise determine a motion and/or displacement of proof mass <NUM>. In other examples (not shown in <FIG>), processing circuitry <NUM> may be part of the feedback loop from MEMS VBA <NUM> and may control the resonator drive signals 106A and 106B to maintain the resonators at their resonant frequency.

In the example of <FIG>, electrode driver circuits 114A and 114B are operatively connected to MEMS VBA <NUM> and may send proof mass actuator electrode drive signals 116A and 116B to MEMS VBA <NUM> as well as receive proof mass actuator electrode sense signals 118A and 118B from MEMS VBA <NUM>. In the example of <FIG>, proof mass actuator electrode driver circuit 114A may be coupled to one electrode, e.g., proof mass actuator electrode 30A depicted in <FIG>, and proof mass actuator electrode driver circuit 114B may be coupled to a second electrode, e.g., proof mass actuator electrode 30B. Alternatively, MEMS VBA <NUM> may be fabricated as part of a wafer including a plurality of accelerometers, and proof mass actuator electrode driver circuits 114A and 114B may be operatively connected to components of the wafer to which MEMS VBA <NUM> may be attached, such as proof mass electrodes 30A and 30B which may be included with the wafer rather than MEMS VBA <NUM>. Proof mass actuator electrode driver circuits 114A and 114B may be configured to output a signal that causes one or more proof mass actuator electrodes to apply a force to a proof mass causing the proof mass to accelerate, displace, vibrate, and/or otherwise move. In some examples, vibrate means to excite and sustain mechanical motion of the proof mass through electrostatic actuation. In some examples, proof mass actuator electrode driver circuits 114A and 114B may include one or more oscillator circuits. In some examples, the signal from proof mass actuator electrode driver circuits 114A and 114B may provide a patterned electric field to cause proof mass <NUM> of MEMS VBA <NUM> to maintain a resonance.

In some examples, proof mass actuator electrode drive circuits 114A and 114B may be configured to adjust the output of proof mass actuator electrode drive signals 116A and 116B based on the feedback loop from proof mass actuator electrode sense signals 118A and 118B, e.g., to maintain proof mass <NUM> at a resonant frequency. A MEMS VBA and/or a wafer including a plurality of MEMS VBAs according to this disclosure may include one proof mass actuator electrode or more than two proof mass actuator electrodes and may also include fewer or additional proof mass actuator electrode driver circuits.

As described above in relation to <FIG>, one or more proof mass actuator electrodes may cause a proof mass of a MEMS VBA to accelerate, displace, vibrate, and/or otherwise move in a direction in a direction substantially parallel to the plane of the proof mass and may cause a rotation of the pendulous proof mass about the hinge flexure parallel to the plane of the proof mass. One or more proof mass actuator electrodes may be configured to sense an acceleration, displacement, vibration, and/or motion of the proof mass. Additionally or alternatively, one or more resonators coupled to a proof mass may be configured to sense an acceleration, displacement, vibration, and/or motion of the proof mass as described above, e.g., the proof mass being driven by one or more proof mass actuator electrodes rather than by an inertial or other force.

For example, a proof mass actuator electrode, e.g., proof mass actuator electrode 30A may be configured to drive the proof mass and one or more other proof mass actuator electrode, e.g., proof mass actuator electrode 30B may be configured to sense the motion of the proof mass. In some examples, proof mass actuator electrode driver circuit 114A may output an oscillating drive signal, such as a sinusoidal voltage drive signal including one or more frequencies. Proof mass actuator electrode driver circuits 114A may be configured to output a sinusoidally oscillating proof mass actuator electrode drive signal 116A that causes proof mass actuator electrode 30A to apply a sinusoidally oscillating force to proof mass <NUM>. The sinusoidally oscillating force may cause proof mass <NUM> to oscillate and/or vibrate, and proof mass actuator electrode 30B may sense the oscillation and/or vibration of proof mass <NUM>, e.g., via an induced current in proof mass actuator electrode 30B proportional to the movement of proof mass <NUM> in an electric field.

Proof mass electrode driver circuit 114A may be configured to output a proof mass actuator electrode drive signal 116A that oscillates at a plurality of frequencies. In some examples, the plurality of frequencies may be applied at the same time, e.g., proof mass actuator electrode drive signal 118A applied to the electrodes may include a plurality of frequency components. In other examples, the plurality of frequencies may be applied over a period of time, e.g., a frequency sweep drive signal. The resulting electrostatic force on proof mass <NUM> may include the plurality of frequencies corresponding to the proof mass actuator electrode drive signal, and proof mass <NUM> may move and/or vibrate in response to the applied oscillating electrostatic force including the plurality of frequencies. In some examples, proof mass <NUM> may move and/or vibrate in resonance with one or more of the plurality of frequencies, e.g., proof mass <NUM> may vibrate with an increased vibration amplitude at the one or more resonant frequencies, for example, one or more proof mass natural frequencies.

In some examples, proof mass actuator electrode 30B may output a proof mass actuator electrode sense signal 118B proportional to the sensed motion of proof mass <NUM>. One or both of proof mass actuator electrode driver circuit 114B and processing circuitry <NUM> may be configured to receive proof mass actuator electrode sense signal 118B and determine the motion of proof mass <NUM>. In some examples, proof mass actuator electrode driver circuit 114B may be configured to drive proof mass <NUM> and proof mass actuator electrode 30A may be configured to sense the motion of proof mass <NUM>.

In some examples, any or all of proof mass actuator electrode driver circuits 114A and 114B and processing circuitry <NUM> may be configured to determine a quality factor (Q) associated with the sensed proof mass natural frequency.

In some examples, resonator driver circuits 104a and 104B and/or processing circuitry <NUM> may be configured to determine an acceleration, a displacement, and/or a motion of proof mass <NUM> caused by one or both of proof mass actuator electrodes 30A and 30B based on one or both of resonator sense signals 108A and 108B.

For example, one or both of proof mass actuator electrode driver circuits 114A and 114B may be configured to output a slowly varying and/or DC signal causing one or both of proof mass actuator electrodes 30A and 30B to create an electrostatic force on proof mass <NUM>. Proof mass <NUM> may displace in response to the applied electrostatic force, and a differential frequency measurement may be determined, e.g., by any of resonator driver circuits 104A and 104B and processing circuitry <NUM> based on resonator sense signals 108A and 108B. Additionally or alternatively, a frequency change of one or both of resonators 18A and 18B may be observed to determine a scale factor in Hz/g. For example, any of resonator driver circuits 104A and 104B and processing circuitry <NUM> may determine a frequency change in one or both of resonators 18A and 18B and based on resonator sense signals 108A and 108B and any of resonator driver circuits 104A and 104B and processing circuitry <NUM> may determine a scale factor based on the determined frequency change.

Processing circuitry <NUM> may communicate with proof mass actuator electrode driver circuits 114A and 114B. Processing circuitry <NUM> may include various signal processing functions, such as filtering, amplification and analog-to-digital conversion (ADC). Filtering functions may include high-pass, band-pass, or other types of signal filtering. In some examples, proof mass actuator electrode driver circuits 114A and 114B may also include signal processing functions, such as amplification and filtering. Processing circuitry <NUM> may output the processed signal received from MEMS VBA <NUM> and/or proof mass actuator electrodes 30A and 30B to other circuitry <NUM> as an analog or digital signal. Processing circuitry <NUM> may also receive signals from other circuitry <NUM>, such as command signals, calibration signals and similar signals.

Processing circuitry <NUM> may operatively connect to MEMS VBA <NUM> and/or a wafer including a plurality of MEMS VBAs <NUM>, e.g., via proof mass actuator electrode driver circuits 114A and 114B. Processing circuitry <NUM> may be configured to receive the signal from MEMS VBA <NUM> and/or a wafer including a plurality of MEMS VBAs <NUM>, which may indicate an acceleration, a motion, a natural frequency, and/or a Q of at least one proof mass of at least one MEMS VBA <NUM>, and may indicate whether at least one proof mass of at least one MEMS VBA is functioning correctly and/or is correctly connected to resonators to cause expected frequency shifts due to acceleration.

In some examples, any or all of electrode driver circuits 114A and 114B, resonator driver circuits 104A and 104B, and processing circuitry <NUM> may be configured to determine whether the proof mass <NUM> is stuck or functioning correctly, and whether the proof mass <NUM> is correctly connected to the resonators, e.g., resonators 18A and 18B, based on any or all of proof mass actuator electrode sense signals 118A and 118B and resonator sense signals 108A and 108B. In some examples, any or all of electrode driver circuits 114A and 114B, resonator driver circuits 104A and 104B, and processing circuitry <NUM> may be configured to determine proof mass characteristics, e.g., one or more proof mass resonant and/or natural frequencies via applying a frequency sweep drive signal to proof mass actuator electrodes 30A and/or 30B.

In some examples, any or all of electrode driver circuits 114A and 114B, resonator driver circuits 104A and 104B, and processing circuitry <NUM> may be configured to calibrate MEMS VBA <NUM> at power-on or at any time during operation. For example, electrode driver circuits 114A and/or 114B may output a signal that causes proof mass actuator electrodes 30A and/or 30B, respectively, to apply a force to proof mass <NUM> causing proof mass <NUM> to move. Proof mass actuator electrodes 30A and/or 30B and resonators 18A and/or 18B to sense the movement of proof mass <NUM> and output proof mass actuator electrode sense signals 118A and/or 118B and/or resonator sense signals 108A and/or 108B, respectively. Electrode driver circuits 114A and/or 114B, or resonator driver circuits 104A and/or 104B, or processing circuitry <NUM>, as appropriate, may then determine a bias and/or scale factor of resonators 18A and/or 18B, and/or one or more calibration parameters of MEMS VBA <NUM>. In other examples, any or all of electrode driver circuits 114A and 114B, resonator driver circuits 104A and 104B, and processing circuitry <NUM> may be configured to calibrate MEMS VBA <NUM> via a frequency sweep drive signal applied to proof mass actuator electrodes 30A and/or 30B. In some examples, any or all of electrode driver circuits 114A and 114B, resonator driver circuits 104A and 104B, and processing circuitry <NUM> may be configured to calibrate MEMS VBA <NUM> periodically and/or or continuously.

In some examples, any or all of electrode driver circuits 114A and 114B, resonator driver circuits 104A and 104B, and processing circuitry <NUM> may be configured to force rebalancing or a force-to-rebalance mode of operation. For example, electrode driver circuits 114A and/or 114B may be configured to apply a DC or slowly varying bias voltage signal to proof mass actuator electrodes 30A and/or 30B that causes to proof mass actuator electrodes 30A and/or 30B to apply a force to proof mass <NUM> to move proof mass <NUM> back to a default position and/or "hold" proof mass <NUM> to a default position, e.g., by applying a force via proof mass actuator electrodes 30A and/or 30B that resists motion of proof mass <NUM> from the default position and thereby causing a greater force (for example, due to acceleration of MEMS VBA <NUM>) to be needed to displace and/or move proof mass <NUM> from the default position. In some examples, system <NUM> may be operated in a closed-loop and/or a feedback loop mode. For example, a force may cause proof mass <NUM> to accelerate, displace, vibrate, or otherwise move, and resonators 18A and/or 18B and/or proof mass electrodes 30A and/or 30B may sense the motion of proof mass <NUM>. Any of electrode driver circuits 114A and/or 114B, or resonator driver circuits 104A and/or 104B, or processing circuitry <NUM> may determine a signal to apply to proof mass actuator electrodes 30A and/or 30B to drive proof mass <NUM> back to a default position, e.g., a zero-g or zero external force position, and may cause electrode driver circuits 114A and/or 114B to apply that signal to proof mass actuator electrodes 30A and 30B. In some examples, resonator driver circuits 104A and/or 104B, or processing circuitry <NUM> may determine a signal to apply to proof mass actuator electrodes 30A and/or 30B to drive proof mass <NUM> back to a default position based on a difference frequency of resonators 18A and 18B, a weighted and/or scaled difference frequency of resonators 18A and 18B, a squared weighted and scaled difference frequency of resonators 18A and 18B, and the like. In some examples, force rebalancing or force-to-rebalance may improve the operation of system <NUM> and/or MEMS VBA <NUM>, e.g., system <NUM> may have an increased sensitivity and/or an extended dynamic range to sense larger forces that may otherwise cause proof mass <NUM> to reach a displacement limit and/or resonators 18A and/or 18B and/or proof mass actuator electrodes 30A and/or 30B to reach a sensing limit.

<FIG> is a flow diagram illustrating an example method <NUM> of testing a MEMS VBA, according to one or more techniques of this disclosure. While method <NUM> is described with reference to MEMS VBA <NUM> and/or a wafer including a plurality of MEMS VBAs <NUM> and electrodes 30A and 30B, the method <NUM> may be used with other sensors.

A proof mass actuator electrode may apply a force to a proof mass with a drive signal including one or more frequencies (<NUM>). In some examples, a proof mass of a MEMS VBA may be driven by a proof mass actuator electrode included with the MEMS VBA or included with a wafer including the MEMS VBA. For example, proof mass actuator electrode driver circuit 114A may output a proof mass actuator electrode drive signal 116A, such as a sinusoidal drive signal including one or more frequencies that causes proof mass actuator electrode 30A to apply a sinusoidally oscillating force to proof mass <NUM>. In some examples, proof mass actuator electrode 30A may apply a force including the plurality of frequencies to proof mass <NUM> at the same time, e.g., proof mass actuator electrode drive signal 118A may include a plurality of frequency components. In other examples, proof mass actuator electrode 30A may apply a force including the plurality of frequencies to proof mass <NUM> over a period of time, e.g., a frequency sweep drive signal. The resulting electrostatic force on proof mass <NUM> may include the plurality of frequencies corresponding to the proof mass actuator electrode drive signal, and proof mass <NUM> may move and/or vibrate in response to the applied oscillating electrostatic force including the plurality of frequencies. In some examples, proof mass <NUM> may move and/or vibrate in resonance with one or more of the plurality of frequencies, e.g., proof mass <NUM> may vibrate with an increased vibration amplitude at the one or more resonant frequencies and/or one or more proof mass natural frequencies.

A proof mass actuator electrode may sense and/or detect a motion of the proof mass in response to the driving force (<NUM>). For example, proof mass actuator electrode 30B may sense the oscillation and/or vibration of proof mass <NUM>. In some examples, proof mass actuator electrode 30B may output a proof mass actuator electrode sense signal 118B proportional to the sensed motion of proof mass <NUM>. One or both of proof mass actuator electrode driver circuit 114B and processing circuitry <NUM> may be configured to receive proof mass actuator electrode sense signal 118B and determine the motion of proof mass <NUM>. In some examples, proof mass actuator electrode driver circuit 114B may be configured to drive proof mass <NUM> and proof mass actuator electrode 30A may be configured to sense the motion of proof mass <NUM>.

One or more proof mass actuator electrodes may be connected to ground (<NUM>). For example, proof mass actuator electrodes may be intended for use only during interim testing such as wafer-level probe testing and package testing. A circuit board (not shown), e.g., including any or all of electrode drive circuitry 114A and 114B, resonator drive circuitry 104A and 104B, processing circuitry <NUM>, and other processing circuitry <NUM>, may connect proof mass actuator electrodes 30A and 30B to ground subsequent to testing such that only inertial forces act upon the proof mass. In other words, electrodes 30A and 30B may be grounded and prevented from acting on or applying a force to proof mass <NUM> when MEMS VBA <NUM> is in use after testing.

<FIG> is a flow diagram illustrating another example method <NUM> of testing a MEMS VBA, according to one or more techniques of this disclosure. While method <NUM> is described with reference to MEMS VBA <NUM> and/or a wafer including a plurality of MEMS VBAs <NUM> and electrodes 30A and 30B, the method <NUM> may be used with other sensors.

A proof mass actuator electrode may apply a force to a proof mass with a DC, or slowly varying, drive signal (<NUM>). In some examples, a proof mass of a MEMS VBA may be driven by a proof mass actuator electrode included with the MEMS VBA or included with a wafer including the MEMS VBA. For example, proof mass actuator electrode driver circuits 114A and 114B may output a proof mass actuator electrode drive signals 116A and 116B, slowly varying and/or DC voltage signal causing one or both of proof mass actuator electrodes 30A and 30B to create an electrostatic force on proof mass <NUM>. Proof mass <NUM> may accelerate, displace, or otherwise move in response to the applied electrostatic force. In some examples, one or both of proof mass actuator electrodes 30A and 30B may displace proof mass <NUM> by a predetermined distance via creating an electrostatic force on proof mass <NUM>.

A resonator may sense and/or detect an acceleration, displacement, and/or a motion of the proof mass in response to the driving force (<NUM>). For example, any of resonator driver circuits 104A and 104B and processing circuitry <NUM> may determine a differential frequency based on resonator sense signals 108A and 108B. Additionally or alternatively, any of resonator driver circuits 104A and 104B and processing circuitry <NUM> may determine a frequency change of one or both of resonators 18A and 18B and determine a scale factor in Hz/g based on the frequency change.

One or more proof mass actuator electrodes may be connected to ground (<NUM>), e.g., similar to (<NUM>) described above. For example, proof mass actuator electrodes may be intended for use only during interim testing such as wafer-level probe testing and package testing. A circuit board (not shown), e.g., including any or all of electrode drive circuitry 114A and 114B, resonator drive circuitry 104A and 104B, processing circuitry <NUM>, and other processing circuitry <NUM>, may connect proof mass actuator electrodes 30A and 30B to ground subsequent to testing such that only inertial forces act upon the proof mass. In other words, electrodes 30A and 30B may be grounded and prevented from acting on or applying a force to proof mass <NUM> when MEMS VBA <NUM> is in use after testing.

The techniques described in this disclosure may be implemented, at least in part, in hardware, software, firmware, or any combination thereof. A control unit including hardware may also perform one or more of the techniques of this disclosure.

Such hardware, software, and firmware may be implemented within the same device or within separate devices to support the various techniques described in this disclosure. Depiction of different features as modules or units is intended to highlight different functional aspects and does not necessarily imply that such modules or units must be realized by separate hardware, firmware, or software components. Rather, functionality associated with one or more modules or units may be performed by separate hardware, firmware, or software components, or integrated within common or separate hardware, firmware, or software components.

The techniques described in this disclosure may also be embodied or encoded in an article of manufacture including a computer-readable storage medium encoded with instructions. Instructions embedded or encoded in an article of manufacture including a computer-readable storage medium, may cause one or more programmable processors, or other processors, to implement one or more of the techniques described herein, such as when instructions included or encoded in the computer-readable storage medium are executed by the one or more processors. Computer readable storage media may include random access memory (RAM), read only memory (ROM), programmable read only memory (PROM), erasable programmable read only memory (EPROM), electronically erasable programmable read only memory (EEPROM), flash memory, a hard disk, a compact disc ROM (CD-ROM), a floppy disk, a cassette, magnetic media, optical media, or other computer readable media. In some examples, an article of manufacture may include one or more computer-readable storage media.

In some examples, a computer-readable storage medium may include a non-transitory medium. The term "non-transitory" may indicate that the storage medium is not embodied in a carrier wave or a propagated signal. In certain examples, a non-transitory storage medium may store data that can, over time, change (e.g., in RAM or cache).

Claim 1:
A system (<NUM>) comprising:
a microelectromechanical system, MEMS, vibrating beam accelerometer, VBA, (<NUM>, <NUM>) comprising:
a proof mass (<NUM>); and
a first resonator (18a) mechanically coupled to the proof mass (<NUM>);
a first electrode (30A) configured to apply a force to the proof mass (<NUM>),
a second electrode (30B) configured to sense a motion of the proof mass (<NUM>) and output a signal corresponding to the sensed motion of the proof mass (<NUM>), and
a circuit board configured to connect the first and second electrodes (30A, 30B) to ground.