阅读说明：本技术 基于隧道磁阻检测的静电刚度调节z轴谐振式微加速度计 (Electrostatic rigidity adjustment Z-axis resonant micro-accelerometer based on tunnel magnetic resistance detection ) 是由 张瑞 王旭虎 于 2020-06-18 设计创作，主要内容包括：基于隧道磁阻检测的静电刚度调节Z轴谐振式微加速度计,包括：支撑框架,键合基板,扭转支撑梁,扭转质量块,谐振质量块,磁阻元件,固定刚度调节电极,可动刚度调节电极,检测磁体和驱动磁体；支撑框架设置在键合基板上,扭转质量块设置在支撑框架上开设的第一质量块安装槽内,扭转质量块通过扭转支撑梁与支撑框架连接；谐振质量块设置在扭转质量块上开设的第二质量块安装槽内,谐振质量块的四个边角通过驱动组合梁与扭转质量块连接,磁阻元件设置在谐振质量块上,谐振质量块的X轴两端设置可动刚度调节电极；键合基板上设置有固定刚度调节电极,检测磁体和驱动磁体,分别对应调节电极露出孔、磁阻元件、驱动组合梁的位置设置。(Static rigidity adjustment Z axle resonant type micro accelerometer based on tunnel magnetic resistance detects includes: the device comprises a supporting frame, a bonding substrate, a torsional supporting beam, a torsional mass block, a resonant mass block, a magnetoresistive element, a fixed rigidity adjusting electrode, a movable rigidity adjusting electrode, a detection magnet and a driving magnet; the support frame is arranged on the bonding substrate, the torsion mass block is arranged in a first mass block mounting groove formed in the support frame, and the torsion mass block is connected with the support frame through the torsion support beam; the resonance mass block is arranged in a second mass block mounting groove formed in the torsion mass block, four corners of the resonance mass block are connected with the torsion mass block through a driving combination beam, the magneto-resistive element is arranged on the resonance mass block, and movable rigidity adjusting electrodes are arranged at two ends of an X axis of the resonance mass block; the bonded substrate is provided with a fixed rigidity adjusting electrode, a detection magnet and a driving magnet which are respectively arranged corresponding to the positions of the adjusting electrode exposure hole, the magnetoresistive element and the driving combination beam.)

1. Static rigidity adjusts Z axle resonance type micro accelerometer based on tunnel magnetic resistance detects, its characterized in that includes: a support frame (1), a bonding substrate (27), a torsion support beam (2), a torsion mass (3), resonance masses (4, 5), magnetoresistive elements (10, 13), fixed stiffness adjustment electrodes (6, 8, 9), movable stiffness adjustment electrodes (7a, 7b, 7c, 7d), detection magnets (28, 29) and drive magnets (30, 31, 32, 33);

the support frame (1) is arranged on the bonding substrate (27), a first mass block mounting groove which is asymmetrically arranged by taking a Y-axis central line of the support frame (1) as a central axis is formed in the support frame (1), the torsion mass block (3) is matched with the shape of the first mass block mounting groove and arranged in the first mass block mounting groove, and the torsion mass block (3) is connected with the support frame (1) through a torsion support beam (2);

two second mass block mounting grooves are symmetrically formed in the torsion mass block (3) along the Y-axis central line of the supporting frame (1) as a central axis, and adjusting electrode exposure holes are formed between the two second mass block mounting grooves and on the two sides of the two second mass block mounting grooves respectively; the resonant mass blocks (4 and 5) are arranged in the second mass block mounting grooves, four corners of the resonant mass blocks (4 and 5) are connected with the torsional mass block (3) through driving combination beams, the magneto-resistive elements (10 and 13) are arranged on the resonant mass blocks (4 and 5), and the movable rigidity adjusting electrodes (7a, 7b, 7c and 7d) are arranged at two ends of an X axis of the resonant mass blocks (4 and 5);

the upper surface of the bonding substrate (27) is provided with a square groove, the fixed rigidity adjusting electrodes (6, 8 and 9), the detecting magnets (28 and 29) and the driving magnets (30, 31, 32 and 33) are arranged in the groove, the fixed rigidity adjusting electrodes (6, 8 and 9) are arranged corresponding to the positions of the exposed holes of the adjusting electrodes and are in cross fit with the movable rigidity adjusting electrodes (7a, 7b, 7c and 7d), the detecting magnets (28 and 29) are arranged corresponding to the positions of the magnetic resistance elements (10 and 13), and the driving magnets (30, 31, 32 and 33) are arranged corresponding to the positions of the driving combination beam.

2. The electrostatic stiffness tuned Z-axis resonant micro-accelerometer based on tunnel magnetoresistive sensing according to claim 1, characterized in that the torsion supporting beam (2) is located on the Y-axis centerline of the supporting frame (1).

3. The electrostatic stiffness tuned Z-axis resonant micro-accelerometer based on tunneling magneto-resistance sensing according to claim 1, wherein a flux concentrating unit is deposited over the sensing magnets (28, 29), the flux concentrating unit shape comprising a triangle or a square.

4. The electrostatic stiffness-adjusted Z-axis resonant micro-accelerometer based on tunneling magnetoresistance detection according to claim 1, wherein the fixed stiffness-adjusting electrodes (6, 8, 9) and the movable stiffness-adjusting electrodes (7a, 7b, 7c, 7d) are both comb-tooth electrodes, and comb-tooth portions of the fixed stiffness-adjusting electrodes (6, 8, 9) and the movable stiffness-adjusting electrodes (7a, 7b, 7c, 7d) are in cross fit.

5. The electrostatic stiffness tuned Z-axis resonant micro-accelerometer based on tunneling magneto-resistance sensing according to claim 1, wherein the drive composite beam comprises: a first drive beam (24a, 24b, 24c, 24d), a second drive beam (26a, 26b, 26c, 26d) and a drive beam connection block (25a, 25b, 25c, 25d), the first driving beams (24a, 24b, 24c, 24d) and the second driving beams (26a, 26b, 26c, 26d) are respectively arranged on two sides of the driving beam connecting blocks (25a, 25b, 25c, 25d) in parallel and one end of each driving beam connecting block (25a, 25b, 25c, 25d) is respectively connected with the driving beam connecting blocks (25a, 25b, 25c, 25d), the other ends of the first driving beams (24a, 24b, 24c, 24d) and the second driving beams (26a, 26b, 26c, 26d) are respectively connected with the resonant masses (4, 5), the other end of the drive beam connecting block (25a, 25b, 25c, 25d) is connected with the torsion mass (3).

6. The electrostatic stiffness tuned Z-axis resonant micro-accelerometer based on tunneling magneto-resistive sensing according to claim 1, further comprising: drive electrodes (16, 18, 20, 22), drive leads (17, 19, 21, 23), sense electrodes (12, 15) and sense leads (11, 14);

the driving electrodes (16, 18, 20, 22) and the detection electrodes (12, 15) are arranged on the upper surface of the torsion mass block (3) close to the edge position of the torsion support beam (2);

two ends of the driving leads (17, 19, 21 and 23) are respectively connected with the positive electrode and the negative electrode of the driving electrodes (16, 18, 20 and 22), the middle parts of the driving leads (17, 19, 21 and 23) are arranged on the driving combination beam, one ends of the detection leads (11 and 14) are connected with the detection electrodes (12 and 15), and the other ends of the detection leads (11 and 14) are connected with the tunnel magneto-resistive elements (10 and 13).

Technical Field

The invention relates to a resonant micro accelerometer device for adjusting Z-axis static stiffness based on tunnel magnetic resistance detection, belonging to the technical field of measuring instrument parts of micro inertial navigation.

Background

The inertia technology works in a completely autonomous mode, is not in contact with the outside, and has the advantages of autonomy, real time and no interference. The gyroscope is a core device of an inertial navigation technology and plays a vital role in the fields of modern aerospace, national defense, military and the like.

An accelerometer is one of the most critical components in an inertial navigation system, and is used for measuring the acceleration value of a vehicle, and on the basis of the acceleration value, the speed position information of the vehicle can be obtained through calculation. Inertial navigation and guidance are based on the acceleration of the accelerometer sensitive measurement carrier, so the performance of the accelerometer directly influences the stability of the measurement precision of the whole system and the final navigation precision.

The resonant micro accelerometer measures external acceleration through the frequency change of the resonant cavity, and has the advantages of large dynamic range, high sensitivity and the like, and has anti-interference capability. Most resonant micro-accelerometers currently being investigated are used to measure in-plane acceleration due to the in-plane linear resonator's high linearity, high accuracy and process characteristics compatible with conventional silicon micro-meters. There are few out-of-plane resonant accelerometers that are capable of measuring acceleration in a vertical plane. The structure adopts a magnetic resistance detection mode to realize resolving of natural frequency of the resonant structure. In terms of a driving mode, the electrostatic driving stability is good, but the driving amplitude is small; the electromagnetic drive has the advantages of large drive amplitude, simple structure and the like. In terms of a detection mode, the capacitance detection adopts a comb structure, the displacement resolution is high, but the precision requirement of the comb manufacturing process is extremely high, and the yield is low. The tunnel magnetoresistance effect is based on the spin effect of electrons, a non-magnetic layer of an insulator or a semiconductor is arranged between a magnetic pinning layer and a magnetic free layer, when the magnetization direction of the magnetic free layer is changed under the action of an external field, but the magnetization direction of the pinning layer is not changed, and at the moment, the relative orientation of the magnetization of the two magnetic layers is changed, a large resistance change can be observed on a magnetic tunnel junction crossing an insulating layer, the physical effect is based on the tunneling effect of electrons on the insulating layer, so the tunnel magnetoresistance effect is called as the tunnel magnetoresistance effect, and the tunnel magnetoresistance effect has the advantages of high sensitivity, miniaturization and easiness in detection.

The natural frequency of a single resonator is very sensitive to temperature change, which leads to false signal output, in order to solve the problem of signal detection, the inventor thinks that the tunnel magnetoresistance effect is applied to an accelerometer structure, a double resonance mass block is adopted to eliminate the influence of factors such as temperature, electromagnetic drive is adopted, the static rigidity change is converted into frequency change through the motion of a torsion mass block, the detection of the natural frequency of the resonance structure is realized by adopting a related closed loop detection circuit, so that the acceleration detection is realized, and related products do not appear in the technical field.

By searching the prior art, the prior art 1, namely 'a resonant micro accelerometer based on electrostatic stiffness' (application number is CN201220188370.9), the prior art 2 ', namely a sensitive structure of a resonant accelerometer with electrostatic negative stiffness and a using method thereof' (application number is CN201811617230.7) and the prior art 3 ', namely a silicon micro resonant accelerometer' (application number is CN201410129567.9) is found.

The prior art 1, the prior art 2 and the prior art 3 adopt a capacitance driving and capacitance detection mode, and a capacitance structure is suitable for MEMS (micro-electromechanical systems) process machining, but has the disadvantages of insufficient detection sensitivity and small output signal; the comb capacitor detection mode is adopted, the displacement resolution is high, but with further miniaturization, the comb voltage is easy to break down, the pick-up failure can be caused during the transverse impact, and particularly, the comb manufacturing process has extremely high precision requirement and low yield, so the development in the direction is restricted.

Based on the problems, the invention provides the resonant micro-accelerometer device adopting the electromagnetic driving and tunnel magnetic resistance detection modes. When in detection, the magnetic resistance element with high sensitivity is used for detection, the sensitivity is high, the process requirement is not high, and the manufacture is easy.

Disclosure of Invention

The invention aims to overcome the defects of the background technology, designs an electrostatic rigidity adjusting Z-axis resonance type micro accelerometer based on tunnel magnetic resistance detection, improves the detection precision of the accelerometer, adopts an electromagnetic driving and magnetic resistance detection mode, changes the electrostatic rigidity of a resonance structure through inputting acceleration, thereby causing the natural frequency of the resonance structure to change, and realizes the detection of the acceleration through detecting the natural frequency of the resonance structure.

The technical scheme of the invention is as follows:

static rigidity adjustment Z axle resonant type micro accelerometer based on tunnel magnetic resistance detects includes: the device comprises a supporting frame, a bonding substrate, a torsional supporting beam, a torsional mass block, a resonant mass block, a magnetoresistive element, a fixed rigidity adjusting electrode, a movable rigidity adjusting electrode, a detection magnet and a driving magnet;

the support frame is arranged on the bonding substrate, a first mass block mounting groove which is asymmetrically arranged by taking a Y-axis central line of the support frame as a central axis is formed in the support frame, the torsion mass block is matched with the shape of the first mass block mounting groove and is arranged in the first mass block mounting groove, and the torsion mass block is connected with the support frame through a torsion support beam;

two second mass block mounting grooves are symmetrically formed in the torsion mass block along the Y-axis central line of the supporting frame as a central axis, and adjusting electrode exposure holes are formed between the two second mass block mounting grooves and on the two sides of the two second mass block mounting grooves respectively; the resonant mass block is arranged in the second mass block mounting groove, four corners of the resonant mass block are connected with the torsional mass block through driving combination beams, the magneto-resistive elements are arranged on the resonant mass block, and the movable rigidity adjusting electrodes are arranged at two ends of an X axis of the resonant mass block;

the upper surface of the bonding substrate is provided with a square groove, the fixed rigidity adjusting electrode, the detection magnet and the driving magnet are arranged in the groove, the fixed rigidity adjusting electrode is arranged corresponding to the position of the adjusting electrode exposing hole and is in cross fit with the movable rigidity adjusting electrode, the detection magnet is arranged corresponding to the position of the magnetic resistance element, and the driving magnet is arranged corresponding to the position of the driving combination beam.

Optionally, the torsion support beam is located on a Y-axis centerline of the support frame.

Optionally, a magnetism gathering unit is deposited above the detection magnet, and the shape of the magnetism gathering unit comprises a triangle or a square.

Optionally, the fixed stiffness adjusting electrode and the movable stiffness adjusting electrode are both comb teeth electrodes, and comb teeth of the fixed stiffness adjusting electrode and comb teeth of the movable stiffness adjusting electrode are in cross fit.

Optionally, the drive combination beam comprises: the driving device comprises a first driving beam, a second driving beam and a driving beam connecting block, wherein the first driving beam and the second driving beam are respectively arranged on two sides of the driving beam connecting block in parallel, one end of the first driving beam is respectively connected with the driving beam connecting block, the other end of the first driving beam and the other end of the second driving beam are respectively connected with the resonance mass block, and the other end of the driving beam connecting block is connected with the torsion mass block.

Optionally, the electrostatic stiffness adjustment Z-axis resonant micro accelerometer based on tunnel magnetoresistance detection further includes: the driving electrode, the driving lead, the detection electrode and the detection lead;

the driving electrode and the detection electrode are arranged on the upper surface of the torsion mass block and close to the edge of the torsion support beam;

the two ends of the driving lead are respectively connected with the positive electrode and the negative electrode of the driving electrode, the middle of the driving lead is arranged on the driving combination beam, one end of the detection lead is connected with the detection electrode, and the other end of the detection lead is connected with the tunnel magnetoresistive element.

The invention provides an electrostatic stiffness adjustment Z-axis resonant micro-accelerometer based on tunnel magnetic resistance detection, which adopts an electromagnetic driving and tunnel magnetic resistance detection mode, simplifies the driving mode, reduces the process difficulty, and simultaneously improves the detection sensitivity. The purpose of detecting the input acceleration is achieved by detecting the change of the natural frequency.

In addition, the invention adopts the double resonance mass blocks, the natural frequency of the single resonance structure is extremely sensitive to temperature change, which can cause false signal output, and the double resonance mass blocks can eliminate the influence of factors such as temperature on the natural frequency. The invention adopts the tunnel magnetic resistance effect with high sensitivity to detect, improves the detection precision of the micro-accelerometer, has high sensitivity to weak magnetic field change by the tunnel magnetic resistance element, can realize more accurate measurement of the natural frequency of the resonant structure, has reasonable structural design and convenient use, and can realize the detection of the Z-axis acceleration by detecting the change of the natural frequency of the resonant structure.

The invention deposits the soft magnetic material of high magnetic conductivity on the detection magnet, have the effect of gathering magnetism, realize and strengthen the local magnetic field intensity thus raise the rate of change of magnetic field, form a kind of stable high rate of change magnetic field, when the magnetic field that the magnetoresistive component of the tunnel senses changes, the resistance value of the magnetoresistive component of the tunnel will change violently under the weak magnetic field change, this change can improve the detection accuracy of the micro-gyro designed by one to two orders of magnitude. The invention has reasonable integral structure design, simple interface circuit and high detection precision.

Drawings

FIG. 1 is a schematic view of the overall structure of the present invention;

FIG. 2 is a top view of the overall structure of the present invention;

FIG. 3 is a schematic view of a bonded substrate structure according to the present invention;

FIG. 4 is a top view of a bonded substrate structure according to the present invention;

FIG. 5 is a schematic view of a torsional mass according to the present invention;

FIG. 6 is a top view of a torsional mass structure according to the present invention;

FIG. 7 is a schematic view of a resonant mass according to the present invention;

FIG. 8 is a top view of the resonating mass structure of the present invention;

FIG. 9 is a schematic view of the structure of the driving electrodes, driving leads, detecting electrodes and detecting leads of the present invention;

FIG. 10 is a top view of the structure of the driving electrodes, driving leads, detecting electrodes and detecting leads of the present invention.

As shown in the figures, the list of reference numbers is as follows:

1-a support frame; 2-twisting the support beam; 3-a torsional mass; 4. 5-a resonant mass block; 6. 8, 9-fixing the stiffness adjusting electrode; 7a, 7b, 7c, 7 d-movable rigidity adjusting electrode; 10. 13-a magnetoresistive element; 11. 14-detection leads; 12. 15-a detection electrode; 16. 18, 20, 22-drive electrodes; 17. 19, 21, 23-drive wires; 24a, 24b, 24c, 24 d-first drive beam; 25a, 25b, 25c, 25 d-drive beam connection block; 26a, 26b, 26c, 26 d-second drive beam; 27-a bonding substrate; 28. 29-a detection magnet; 30. 31, 32, 33-drive magnets.

Detailed Description

Reference will now be made in detail to embodiments of the present invention, examples of which are illustrated in the accompanying drawings, wherein like or similar reference numerals refer to the same or similar elements or elements having the same or similar function throughout. The embodiments described below with reference to the accompanying drawings are illustrative only for the purpose of explaining the present invention, and are not to be construed as limiting the present invention.

In the description of the present invention, it is to be understood that the terms "center", "upper", "lower", "front", "rear", "left", "right", and the like indicate orientations or positional relationships based on those shown in the drawings, and are only for convenience in describing the present invention and simplifying the description, but do not indicate or imply that the combination or element referred to must have a specific orientation, be constructed in a specific orientation, and be operated, and thus, are not to be construed as limiting the present invention. In addition, in the description process of the embodiment of the present invention, the positional relationships of the devices such as "upper", "lower", "front", "rear", "left", "right", and the like in all the drawings are based on fig. 1.

In the description of the present invention, it is to be noted that, unless otherwise explicitly specified or limited, the terms "connected" and "connected" are to be interpreted broadly, e.g., as being fixed or detachable or integrally connected; can be mechanically or electrically connected; they may be connected directly or indirectly through intervening media, or they may be interconnected between two elements. The specific meanings of the above terms in the present invention can be understood in specific cases to those skilled in the art.

The invention is further described below with reference to the accompanying drawings:

as shown in fig. 1 and 2, the electrostatic stiffness adjustment Z-axis resonant micro-accelerometer based on tunnel magnetoresistance detection includes: a support frame 1, a bonded substrate 27, a torsion support beam 2, a torsion mass 3, resonant masses 4, 5, magnetoresistive elements 10, 13, fixed stiffness-adjusting electrodes 6, 8, 9, movable stiffness-adjusting electrodes 7a, 7b, 7c, 7d, detection magnets 28, 29, and drive magnets 30, 31, 32, 33.

As shown in fig. 5 and 6, the supporting frame 1 is disposed on the bonding substrate 27, and the supporting frame 1 is formed with first proof mass mounting slots asymmetrically disposed with a Y-axis center line of the supporting frame 1 as a center axis, where the first proof mass mounting slots include, but are not limited to, T-shapes.

As shown in fig. 1, 2, 5 and 6, the shape of the torsion mass 3 fitting the first mass mounting groove is set in the first mass mounting groove, a gap is provided between the torsion mass 3 and the support frame 1, and the shape of the torsion mass 3 includes, but is not limited to, T-shape. The torsional mass 3 is connected with the support frame 1 through a torsional support beam 2, and the torsional support beam 2 is located on the Y-axis central line of the support frame 1.

As shown in fig. 5 and 6, two second mass block mounting grooves are symmetrically formed in the torsion mass block 3 along the Y-axis central line of the support frame 1 as a central axis, and adjustment electrode exposure holes are respectively formed between the two second mass block mounting grooves and at two sides of the two second mass block mounting grooves.

As shown in fig. 1, 2, 7 and 8, the resonant masses 4 and 5 are disposed in the second mass mounting grooves, four corners of the resonant masses 4 and 5 are connected to the torsional mass 3 through driving composite beams, and the magneto resistive elements 10 and 13 are disposed on the resonant masses 4 and 5. The movable rigidity adjusting electrodes 7a, 7b, 7c, 7d are provided at both ends of the X axis of the resonating masses 4, 5.

As shown in fig. 1 to 4, 7 and 8, the bonded substrate 27 has the same shape as the supporting frame 1, and is square as a whole to provide support for the supporting frame 1. The upper surface of the bonding substrate 27 is provided with a square groove, the fixed stiffness adjustment electrodes 6, 8, 9, the detection magnets 28, 29 and the driving magnets 30, 31, 32, 33 are arranged in the groove, the depth of the groove is greater than the thickness of the detection magnets 28, 29, the fixed stiffness adjustment electrodes 6, 8, 9 are arranged corresponding to the positions of the adjustment electrode exposure holes and are in cross fit with the movable stiffness adjustment electrodes 7a, 7b, 7c, 7d, the fixed stiffness adjustment electrodes 6, 8, 9 are exposed to the same plane matched with the movable stiffness adjustment electrodes 7a, 7b, 7c, 7d through the adjustment electrode exposure holes, the detection magnets 28, 29 are arranged corresponding to the positions of the magnetoresistive elements 10, 13, the driving magnets 30, 31, 32, 33 are arranged corresponding to the positions of the driving combination beam, specifically, the detection magnets 28, 32, 29 are located below the magneto resistive elements 10, 13 and the drive magnets 30, 31, 32, 33 are located below the drive combination beam. The detection magnets 28 and 29 can be permanent magnets, electrified coils, photo-controlled magnets and other devices capable of generating magnetic fields, the permanent magnets are adopted in the embodiment for illustration, the detection magnets 28 and 29 are square and can be obtained by process etching, magnetic gathering units are deposited above the detection magnets 28 and 29, and the magnetic gathering units can be triangular, square and the like. The driving magnets 30, 31, 32, 33 are rectangular parallelepiped permanent magnets.

As shown in fig. 1 to 4, 7, and 8, the fixed stiffness-adjusting electrodes 6, 8, and 9 and the movable stiffness-adjusting electrodes 7a, 7b, 7c, and 7d are comb-teeth electrodes. The comb-tooth parts of the fixed stiffness adjustment electrodes 6, 8, 9 and the movable stiffness adjustment electrodes 7a, 7b, 7c, 7d are in cross fit.

As shown in fig. 1-2, 7 and 8, the driving composite beams are respectively disposed at four corners of the resonant masses 4 and 5, the eight driving composite beams have the same structural size, and the driving composite beams include: first drive beams 24a, 24b, 24c, 24d, second drive beams 26a, 26b, 26c, 26d, and drive beam connection blocks 25a, 25b, 25c, 25d, wherein the first drive beams 24a, 24b, 24c, 24d, the second drive beams 26a, 26b, 26c, 26d are respectively disposed in parallel at two sides of the drive beam connection blocks 25a, 25b, 25c, 25d and have one end connected to the drive beam connection blocks 25a, 25b, 25c, 25d, respectively, the first drive beams 24a, 24b, 24c, 24d, the second drive beams 26a, 26b, 26c, 26d have the other ends connected to the resonant masses 4, 5, respectively, and the drive beam connection blocks 25a, 25b, 25c, 25d have the other ends connected to the torsional masses 3. The first drive beams 24a, 24b, 24c, 24d and the second drive beams 26a, 26b, 26c, 26d are elongated beam structures, i.e. the length of the beams is much larger than its width, and the thickness of the first drive beams 24a, 24b, 24c, 24d and the second drive beams 26a, 26b, 26c, 26d is the same as the thickness of the drive beam connection blocks 25a, 25b, 25c, 25 d.

As shown in fig. 1-2, 9 and 10, the electrostatic stiffness adjusting Z-axis resonant micro accelerometer based on tunnel magnetoresistance detection further includes: drive electrodes 16, 18, 20, 22, drive leads 17, 19, 21, 23, sense electrodes 12, 15 and sense leads 11, 14.

The driving electrodes 16, 18, 20, 22 and the detecting electrodes 12, 15 are disposed on the upper surface of the torsion mass 3 near the edges of the torsion support beam 2.

As shown in fig. 9 and 10, two ends of the driving wires 17, 19, 21, and 23 are respectively connected to the positive and negative electrodes of the driving electrodes 16, 18, 20, and 22, and the middle portions of the driving wires 17, 19, 21, and 23 are disposed on the driving composite beam, and when the driving wires are energized, they are subjected to an ampere force in a magnetic field to generate a driving force. One end of each of the sensing wires 11 and 14 is connected to the sensing electrodes 12 and 15, and the other end of each of the sensing wires 11 and 14 is connected to the tunnel magnetoresistive elements 10 and 13.

The invention principle is as follows:

the electrostatic rigidity adjustment Z-axis resonant micro-accelerometer based on tunnel magnetic resistance detection is driven by an ampere force received by an electrified driving wire in a magnetic field, resonant mass blocks on two sides of the structure reciprocate along a Y axis under a driving mode, and the in-plane driving of the resonant mass blocks vibrating at the natural frequency is realized by applying excitation to driving electrodes.

After the micro-accelerometer device is driven, the resonant mass blocks on two sides respectively reciprocate along the Y-axis direction at the natural frequency, the magnetic resistance elements arranged on the resonant mass blocks can detect the magnetic field change caused by the resonant displacement, and the resonant displacement is fed back to the driving electrode through the closed-loop self-oscillation system to track the natural frequency of the resonator. An applied bias voltage between the fixed stiffness tuning electrode and the movable stiffness tuning electrode on the resonating mass generates an electrostatic force and an electrostatic stiffness.

When a z-axis acceleration is input, the torsional mass will twist around the torsional support beams due to the imbalance of the torsional masses on either side of the torsional mass. The overlapping area of the fixed rigidity adjusting electrode and the movable rigidity adjusting electrode on the resonance mass block is changed, so that the electrostatic force and the electrostatic rigidity of the resonator are changed, and the natural frequency of the resonator is changed due to the change of the electrostatic rigidity. Acceleration can be detected by measuring the frequency change of the closed loop self-oscillating system.

The invention provides an electrostatic stiffness adjustment Z-axis resonant micro-accelerometer based on tunnel magnetic resistance detection, which adopts an electromagnetic driving and tunnel magnetic resistance detection mode, simplifies the driving mode, reduces the process difficulty, and simultaneously improves the detection sensitivity. The purpose of detecting the input acceleration is achieved by detecting the change of the natural frequency.

In addition, the invention adopts the double resonance mass blocks, the natural frequency of the single resonance structure is extremely sensitive to temperature change, which can cause false signal output, and the double resonance mass blocks can eliminate the influence of factors such as temperature on the natural frequency. The invention adopts the tunnel magnetic resistance effect with high sensitivity to detect, improves the detection precision of the micro-accelerometer, has high sensitivity to weak magnetic field change by the tunnel magnetic resistance element, can realize more accurate measurement of the natural frequency of the resonant structure, has reasonable structural design and convenient use, and can realize the detection of the Z-axis acceleration by detecting the change of the natural frequency of the resonant structure.

The invention deposits the soft magnetic material of high magnetic conductivity on the detection magnet, have the effect of gathering magnetism, realize and strengthen the local magnetic field intensity thus raise the rate of change of magnetic field, form a kind of stable high rate of change magnetic field, when the magnetic field that the magnetoresistive component of the tunnel senses changes, the resistance value of the magnetoresistive component of the tunnel will change violently under the weak magnetic field change, this change can improve the detection accuracy of the micro-gyro designed by one to two orders of magnitude. The invention has reasonable integral structure design, simple interface circuit and high detection precision.

In the description herein, references to the description of the term "one embodiment," "some embodiments," "an illustrative embodiment," "an example," "a specific example," or "some examples" or the like mean that a particular feature, structure, material, or characteristic described in connection with the embodiment or example is included in at least one embodiment or example of the invention. In this specification, the schematic representations of the terms used above do not necessarily refer to the same embodiment or example. Furthermore, the particular features, structures, materials, or characteristics described may be combined in any suitable manner in any one or more embodiments or examples.

Although embodiments of the present invention have been shown and described, it will be appreciated by those skilled in the art that changes, modifications, substitutions and alterations can be made in these embodiments without departing from the principles and spirit of the invention, the scope of which is defined in the claims and their equivalents.